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&lt;div&gt;The &#039;&#039;&#039;rigid rotor&#039;&#039;&#039; is a mechanical model that is used to explain rotating systems. &lt;br /&gt;
An arbitrary rigid rotor is a 3-dimensional rigid object, such as a [[top]]. To orient such an object in space three angles known as [[Euler angles]] are required. A special rigid rotor is the linear rotor which requires only two angles to describe its orientation. An example of a linear rotor&lt;br /&gt;
is a diatomic [[molecule]]. More general molecules like water (asymmetric rotor),&lt;br /&gt;
ammonia (symmetric rotor), or methane (spherical rotor) are 3-dimensional, see [[Rotational spectroscopy#Classification of molecules based on rotational behavior|classification of molecules]].&amp;lt;/small&amp;gt;&lt;br /&gt;
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== Linear rotor ==&lt;br /&gt;
The linear rigid rotor model consists of two point masses located at fixed distances from their center of mass. &lt;br /&gt;
The fixed distance between the two masses and the values of the masses are the only characteristics of the rigid model.  However, for many actual diatomics this model is too restrictive since  distances are usually not completely fixed.  Corrections on the rigid model can be made to compensate for small variations in the distance. Even in such a case the rigid rotor model is a useful point of departure (zeroth-order model).&lt;br /&gt;
&lt;br /&gt;
=== Classical linear rigid rotor ===&lt;br /&gt;
The classical linear rotor consists of two point masses &amp;lt;math&amp;gt;m_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;m_2&amp;lt;/math&amp;gt;&lt;br /&gt;
(with  [[reduced mass]] &amp;lt;math&amp;gt;\mu = \frac{m_1m_2}{m_1+m_2}&amp;lt;/math&amp;gt;) each at a distance &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt;. The rotor is rigid if &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt; is independent of time.&lt;br /&gt;
The kinematics of a linear rigid rotor is usually described by means of  [[spherical coordinates|spherical polar coordinates]], which form a coordinate system of &#039;&#039;&#039;R&#039;&#039;&#039;&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;. In the physics convention the coordinates are the co-latitude (zenith) angle &amp;lt;math&amp;gt;\theta \,&amp;lt;/math&amp;gt;, the longitudinal (azimuth) angle &amp;lt;math&amp;gt;\varphi\,&amp;lt;/math&amp;gt; and the distance &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt;.&lt;br /&gt;
The angles specify the orientation of the rotor in space.&lt;br /&gt;
The kinetic energy &amp;lt;math&amp;gt;T&amp;lt;/math&amp;gt; of the linear rigid rotor is given by&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
2T = \mu R^2\big [\dot{\theta}^2+(\dot\varphi\,\sin\theta)^2\big]= \mu R^2 \big(\dot{\theta}\;\; \dot{\varphi} \Big)&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
1 &amp;amp; 0 \\&lt;br /&gt;
0 &amp;amp; \sin^2 \theta \\&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\dot{\theta}\\ \dot{\varphi} &lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
= &lt;br /&gt;
\mu  \Big(\dot{\theta}\;\; \dot{\varphi} \Big)&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
h_\theta^2 &amp;amp; 0 \\&lt;br /&gt;
0 &amp;amp; h_\varphi^2 \\&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\dot{\theta}\\ \dot{\varphi} &lt;br /&gt;
\end{pmatrix},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;h_\theta = R\, &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;h_\varphi= R\sin\theta\,&amp;lt;/math&amp;gt; are &lt;br /&gt;
[[Curvilinear coordinates#Terminology|scale (or Lamé) factors]].&lt;br /&gt;
&lt;br /&gt;
Scale factors are of importance for quantum mechanical applications since they&lt;br /&gt;
enter the [[Laplacian]] expressed in [[Curvilinear coordinates#Grad.2C curl.2C div.2C Laplacian|curvilinear coordinates]].&lt;br /&gt;
In the case at hand (constant &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt;)&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\nabla^2 = \frac{1}{h_\theta h_\varphi}\left[ &lt;br /&gt;
\frac{\partial}{\partial \theta} \frac{h_\varphi}{h_\theta} \frac{\partial}{\partial \theta}&lt;br /&gt;
+\frac{\partial}{\partial \varphi} \frac{h_\theta}{h_\varphi} \frac{\partial}{\partial \varphi}&lt;br /&gt;
\right]=&lt;br /&gt;
 \frac{1}{R^2}\left[\frac{1}{\sin\theta}&lt;br /&gt;
\frac{\partial}{\partial \theta} \sin\theta \frac{\partial}{\partial \theta}&lt;br /&gt;
+\frac{1}{\sin^2\theta}\frac{\partial^2}{\partial \varphi^2} &lt;br /&gt;
\right].&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
The classical Hamiltonian function of the linear rigid rotor is&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
H = \frac{1}{2\mu R^2}\left[p^2_{\theta} + \frac{p^2_{\varphi}}{\sin^2\theta}\right].&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Quantum mechanical linear rigid rotor ===&lt;br /&gt;
The linear rigid rotor model can be used in [[quantum mechanics]] to predict the rotational energy of a [[diatomic]] molecule.  The rotational energy depends on the [[moment of inertia]] for the system, &amp;lt;math&amp;gt;I &amp;lt;/math&amp;gt;.  In the [[center of mass]] reference frame, the moment of inertia is equal to: &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; I = \mu R^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt; is the [[reduced mass]] of the molecule and &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt; is the distance between the two atoms.&lt;br /&gt;
&lt;br /&gt;
According to [[quantum mechanics]], the energy levels  of a system can be determined by solving the [[Schrödinger equation]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\hat H \Psi = E \Psi &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\Psi&amp;lt;/math&amp;gt; is the [[wave function]]  and &amp;lt;math&amp;gt;\hat H&amp;lt;/math&amp;gt; is the energy ([[Hamiltonian (quantum mechanics)|Hamiltonian]]) operator.  For the rigid rotor in a field-free space, the energy operator corresponds to the [[kinetic energy]]&amp;lt;ref name=&amp;quot;Podolsky&amp;quot;&amp;gt;{{cite journal| first=B. |last=Podolsky|journal=Phys. Rev.|volume=32|page=812|year=1928|bibcode = 1928PhRv...32...812J |doi = 10.1103/PhysRev.32.812 }}&amp;lt;/ref&amp;gt; of the system:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\hat H = - \frac{\hbar^2}{2\mu} \nabla^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\hbar&amp;lt;/math&amp;gt; is [[reduced Planck constant]] and &amp;lt;math&amp;gt;\nabla^2&amp;lt;/math&amp;gt; is the [[Laplacian]].  The Laplacian is given above in terms of spherical polar coordinates.  The energy operator written in terms of these coordinates is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\hat H =- \frac{\hbar^2}{2I} \left [ {1 \over \sin \theta} {\partial \over \partial \theta} \left ( \sin \theta {\partial \over \partial \theta} \right ) + {1 \over {\sin^2 \theta}} {\partial^2 \over \partial \varphi^2} \right]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This operator appears also in the Schrödinger equation of the hydrogen atom after the radial part&lt;br /&gt;
is separated off. The eigenvalue equation becomes&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
   \hat H Y_\ell^m (\theta, \varphi ) = \frac{\hbar^2}{2I} \ell(\ell+1) Y_\ell^m (\theta, \varphi ). &lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
The symbol &amp;lt;math&amp;gt;Y_\ell^m (\theta, \varphi )&amp;lt;/math&amp;gt; represents a set of functions known as the [[spherical harmonic]]s. Note that the energy does not depend on &amp;lt;math&amp;gt;m \,&amp;lt;/math&amp;gt;. The energy &lt;br /&gt;
:&amp;lt;math&amp;gt; E_\ell = {\hbar^2 \over 2I} \ell \left (\ell+1\right )&amp;lt;/math&amp;gt;&lt;br /&gt;
is &amp;lt;math&amp;gt;2\ell+1&amp;lt;/math&amp;gt;-fold degenerate: the functions with fixed &amp;lt;math&amp;gt;\ell\,&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;m=-\ell,-\ell+1,\dots,\ell&amp;lt;/math&amp;gt; have the same energy.&lt;br /&gt;
&lt;br /&gt;
Introducing the &#039;&#039;rotational constant&#039;&#039; &#039;&#039;B&#039;&#039;, we write,&lt;br /&gt;
:&amp;lt;math&amp;gt;  E_\ell  = B\; \ell \left (\ell+1\right )\quad&lt;br /&gt;
\textrm{with}\quad B \equiv \frac{\hbar^2}{2I}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
In the units of [[reciprocal length]] the rotational constant is,&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar B \equiv \frac{B}{hc} = \frac{h}{8\pi^2cI}, &amp;lt;/math&amp;gt;&lt;br /&gt;
with &#039;&#039;c&#039;&#039; the speed of light. If [[cgs units]] are used for &#039;&#039;h&#039;&#039;, &#039;&#039;c&#039;&#039;, and &#039;&#039;I&#039;&#039;, &amp;lt;math&amp;gt;\bar B&amp;lt;/math&amp;gt; is expressed&lt;br /&gt;
in  [[Wavenumber|wave numbers]], cm&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;, a unit that is often used for rotational-vibrational spectroscopy.&lt;br /&gt;
The rotational constant &amp;lt;math&amp;gt;\bar B(R)&amp;lt;/math&amp;gt;  depends on the distance &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt;. Often one writes   &amp;lt;math&amp;gt; B_e = \bar B(R_e) &amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;R_e&amp;lt;/math&amp;gt; is the equilibrium value&lt;br /&gt;
of &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt; (the value for which the interaction energy of the atoms in the rotor has  a minimum).&lt;br /&gt;
&lt;br /&gt;
A typical rotational spectrum consists of a series of peaks that correspond to transitions between levels with different values of the angular momentum [[quantum number]] (&amp;lt;math&amp;gt;\ell&amp;lt;/math&amp;gt;).    Consequently, [[Rotational spectroscopy|rotational peaks]] appear at energies corresponding to an integer multiple of &amp;lt;math&amp;gt;2\bar B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
=== Selection rules ===&lt;br /&gt;
Rotational transitions of a molecule occur when the molecule absorbs a photon [a particle of a quantized electromagnetic (em) field]. Depending on the energy of the photon (i.e., the wavelength of the em field)  this transition may be seen as a sideband of a vibrational and/or &lt;br /&gt;
electronic transition. Pure rotational transitions, in which the vibronic (= vibrational plus electronic) wave function does not change, occur in the [[microwave]] region of the electromagnetic spectrum.&lt;br /&gt;
&lt;br /&gt;
Typically, rotational transitions can only be observed when the angular momentum [[quantum number]] changes by 1 (&amp;lt;math&amp;gt;\Delta l = \pm 1&amp;lt;/math&amp;gt;).  This selection rule arises from a first-order perturbation theory approximation of  the [[Schrödinger equation|time-dependent Schrödinger equation]].  According to this treatment, rotational transitions can only be observed when one or more&lt;br /&gt;
components of the [[Dipole#Quantum mechanical dipole operator|dipole operator]]&lt;br /&gt;
have a non-vanishing  transition moment.  If &#039;&#039;z&#039;&#039; is the direction of the electric field component of the incoming electromagnetic wave, the transition moment is,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\langle \psi_2 | \mu_z | \psi_1\rangle =&lt;br /&gt;
\left ( \mu_z \right )_{21} = \int \psi_2^*\mu_z\psi_1\, \mathrm{d}\tau .&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
A transition occurs if this integral is non-zero. By separating  the rotational part of the molecular wavefunction from the vibronic&lt;br /&gt;
part, one can show that this means that the molecule must have a permanent [[Dipole#Molecular dipoles|dipole moment]]. &lt;br /&gt;
After integration over the vibronic coordinates&lt;br /&gt;
the following rotational part of the transition moment remains,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; &lt;br /&gt;
\left ( \mu_z \right )_{l,m;l&#039;,m&#039;} = \mu \int_0^{2\pi} \mathrm{d}\phi \int_0^\pi   Y_{l&#039;}^{m&#039;} \left ( \theta , \phi \right )^* \cos \theta\,Y_l^m\, \left ( \theta , \phi \right )\; \mathrm{d}\cos\theta .&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
Here &amp;lt;math&amp;gt;\mu \cos\theta \, &amp;lt;/math&amp;gt; is the &#039;&#039;z&#039;&#039; component of the permanent dipole moment. The moment &amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt; is the vibronically averaged component of the [[Dipole#Quantum mechanical dipole operator|dipole operator]]. Only the  component of the permanent dipole along the axis of a heteronuclear molecule is non-vanishing.&lt;br /&gt;
By the use of the orthogonality of the [[spherical harmonics]]  &amp;lt;math&amp;gt;Y_l^m\, \left ( \theta , \phi \right )&amp;lt;/math&amp;gt;&lt;br /&gt;
it is possible to determine which values of &amp;lt;math&amp;gt;l&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;m&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;l&#039;&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;m&#039;&amp;lt;/math&amp;gt; will result in nonzero values for the dipole transition moment integral.  This constraint results in the observed selection rules for the rigid rotor:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; &lt;br /&gt;
\Delta m = 0  \quad\hbox{and}\quad  \Delta l = \pm 1 &lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Non-rigid linear rotor ===&lt;br /&gt;
&lt;br /&gt;
The rigid rotor is commonly used to describe the rotational energy of diatomic molecules but it is not a completely accurate description of such molecules.  This is because molecular bonds (and therefore the interatomic distance &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt;) are not completely fixed; the bond between the atoms stretches out as the molecule rotates faster (higher values of the rotational [[quantum number]] &amp;lt;math&amp;gt;l&amp;lt;/math&amp;gt;).  This effect can be accounted for by introducing a correction factor known as the centrifugal distortion constant &amp;lt;math&amp;gt;\bar{D}&amp;lt;/math&amp;gt; (bars on top of various quantities indicate that these quantities are expressed in cm&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar E_l = {E_l \over hc} = \bar {B}l \left (l+1\right ) - \bar {D}l^2 \left (l+1\right )^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar D = {4 \bar {B}^3 \over \bar{\boldsymbol\omega}^2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\bar{\boldsymbol\omega}&amp;lt;/math&amp;gt; is the fundamental vibrational frequency of the bond (in cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;).  This frequency is related to the reduced mass and the [[force constant]] (bond strength) of the molecule according to&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar{\boldsymbol\omega} = {1\over 2\pi c} \sqrt{k \over \mu }&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The non-rigid rotor is an acceptably accurate model for diatomic molecules but is still somewhat imperfect.  This is because, although the model does account for bond stretching due to rotation, it ignores any bond stretching due to vibrational energy in the bond (anharmonicity in the potential).&lt;br /&gt;
&lt;br /&gt;
== Arbitrarily shaped rigid rotor ==&lt;br /&gt;
An arbitrarily shaped rigid rotor is a [[rigid body]] of arbitrary shape with its [[center of mass]] fixed (or in uniform rectilinear motion) in field-free space &#039;&#039;&#039;R&#039;&#039;&#039;&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;, so that its energy consists only of rotational kinetic energy (and possibly constant translational energy that can be ignored).  A rigid body can be (partially) characterized by the three eigenvalues of its [[moment of inertia tensor]], which are real nonnegative values known as &#039;&#039;principal moments of inertia&#039;&#039;.&lt;br /&gt;
In [[microwave spectroscopy]]&amp;amp;mdash;the spectroscopy based on rotational transitions&amp;amp;mdash;one usually classifies molecules (seen as rigid rotors) as follows:&lt;br /&gt;
* spherical rotors&lt;br /&gt;
* symmetric  rotors&lt;br /&gt;
** oblate symmetric rotors&lt;br /&gt;
** prolate symmetric rotors&lt;br /&gt;
* asymmetric rotors&lt;br /&gt;
This classification depends on the [[Microwave spectroscopy#Classification of molecules based on rotational behavior|relative magnitudes]] of the principal moments of inertia.&lt;br /&gt;
&lt;br /&gt;
=== Coordinates of the rigid rotor ===&lt;br /&gt;
&lt;br /&gt;
Different branches of physics and engineering use different coordinates for the description&lt;br /&gt;
of the kinematics of a rigid rotor. In molecular physics  [[Euler angles]] are used almost exclusively. In quantum mechanical applications it is advantageous to use Euler&lt;br /&gt;
angles in a convention that is a simple extension of the physical convention of  [[Spherical coordinate system|spherical polar coordinates]]. &lt;br /&gt;
&lt;br /&gt;
The first step is the attachment of a &#039;&#039;&#039;right-handed&#039;&#039;&#039; orthonormal  frame (3-dimensional system of orthogonal axes) to the rotor (a &#039;&#039;&#039;body-fixed frame&#039;&#039;&#039;) . This frame can be attached arbitrarily to the body, but often one uses the principal axes frame&amp;amp;mdash;the normalized eigenvectors of the inertia tensor, which always can be chosen orthonormal, since the tensor is [[Hermitian matrix|Hermitian]]. When the rotor possesses a  symmetry-axis, it usually coincides with one of the principal axes. It is convenient to choose&lt;br /&gt;
as body-fixed &#039;&#039;z&#039;&#039;-axis the highest-order symmetry axis.&lt;br /&gt;
&lt;br /&gt;
One starts by aligning the body-fixed frame with a &#039;&#039;&#039;space-fixed frame&#039;&#039;&#039;&lt;br /&gt;
(laboratory axes), so that the body-fixed &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039;, and &#039;&#039;z&#039;&#039; axes coincide with the space-fixed &#039;&#039;X&#039;&#039;, &#039;&#039;Y&#039;&#039;, and &#039;&#039;Z&#039;&#039; axis. Secondly, the body and its frame are  rotated &#039;&#039;&#039;actively&#039;&#039;&#039; over a &#039;&#039;&#039;positive angle&#039;&#039;&#039; &amp;lt;math&amp;gt;\alpha\,&amp;lt;/math&amp;gt; around the &#039;&#039;z&#039;&#039;-axis (by the [[Right-hand rule#Direction associated with a rotation|right-hand rule]]), which moves the &amp;lt;math&amp;gt;y&amp;lt;/math&amp;gt;-  to the &amp;lt;math&amp;gt;y&#039;&amp;lt;/math&amp;gt;-axis. Thirdly, one rotates the body and its frame over a positive angle &amp;lt;math&amp;gt;\beta\,&amp;lt;/math&amp;gt; around the &amp;lt;math&amp;gt;y&#039;&amp;lt;/math&amp;gt;-axis. The &#039;&#039;z&#039;&#039;-axis of the body-fixed frame has after these two rotations the longitudinal angle &amp;lt;math&amp;gt;\alpha \,&amp;lt;/math&amp;gt; (commonly designated by &amp;lt;math&amp;gt;\varphi\,&amp;lt;/math&amp;gt;) and the colatitude angle &amp;lt;math&amp;gt;\beta\,&amp;lt;/math&amp;gt; (commonly designated by &amp;lt;math&amp;gt;\theta\,&amp;lt;/math&amp;gt; ), both with respect to the space-fixed frame. If the rotor were cylindrical symmetric around its &#039;&#039;z&#039;&#039;-axis, like the linear rigid rotor, its orientation in space would be unambiguously specified at this point.&lt;br /&gt;
&lt;br /&gt;
If the body lacks cylinder (axial) symmetry, a last rotation around its &#039;&#039;z&#039;&#039;-axis (which has polar coordinates &amp;lt;math&amp;gt;\beta\,&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\alpha\,&amp;lt;/math&amp;gt; ) is necessary to specify its orientation completely. Traditionally the last rotation angle is called &amp;lt;math&amp;gt;\gamma\,&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The [[Euler angles#Conventions|convention for Euler angles]] described here is known as the &amp;lt;math&amp;gt;z&#039;&#039;-y&#039;-z&amp;lt;/math&amp;gt; convention; it can be shown (in the same manner as in [[Euler angles#Definition|this article]]) that it is equivalent to the &amp;lt;math&amp;gt;z-y-z&amp;lt;/math&amp;gt; convention in which the order of rotations is reversed.&lt;br /&gt;
&lt;br /&gt;
The total matrix of the three consecutive  rotations  is the product&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\mathbf{R}(\alpha,\beta,\gamma)=&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\cos\alpha &amp;amp; -\sin\alpha &amp;amp; 0 \\&lt;br /&gt;
\sin\alpha &amp;amp; \cos\alpha  &amp;amp; 0 \\&lt;br /&gt;
    0      &amp;amp;      0      &amp;amp; 1&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\cos\beta  &amp;amp;   0  &amp;amp; \sin\beta  \\&lt;br /&gt;
     0     &amp;amp;   1  &amp;amp;        0 \\  &lt;br /&gt;
-\sin\beta &amp;amp;   0  &amp;amp; \cos\beta  \\&lt;br /&gt;
 \end{pmatrix}&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\cos\gamma &amp;amp; -\sin\gamma &amp;amp; 0 \\&lt;br /&gt;
\sin\gamma &amp;amp; \cos\gamma  &amp;amp; 0 \\&lt;br /&gt;
    0      &amp;amp;      0      &amp;amp; 1&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;\mathbf{r}(0)&amp;lt;/math&amp;gt; be the coordinate vector of an arbitrary point &amp;lt;math&amp;gt;\mathcal{P}&amp;lt;/math&amp;gt; in the body  with respect to the body-fixed frame. The elements of &amp;lt;math&amp;gt;\mathbf{r}(0)&amp;lt;/math&amp;gt; are the &#039;body-fixed coordinates&#039; of &amp;lt;math&amp;gt;\mathcal{P}&amp;lt;/math&amp;gt;. Initially &amp;lt;math&amp;gt;\mathbf{r}(0)&amp;lt;/math&amp;gt; is also the space-fixed coordinate vector of &amp;lt;math&amp;gt;\mathcal{P}&amp;lt;/math&amp;gt;.&lt;br /&gt;
Upon rotation of the body, the body-fixed coordinates of &amp;lt;math&amp;gt;\mathcal{P}&amp;lt;/math&amp;gt; do not change, but the space-fixed coordinate vector of &amp;lt;math&amp;gt;\mathcal{P}&amp;lt;/math&amp;gt;   becomes,  &lt;br /&gt;
:&amp;lt;math&amp;gt; &lt;br /&gt;
\mathbf{r}(\alpha,\beta,\gamma)= \mathbf{R}(\alpha,\beta,\gamma)\mathbf{r}(0).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
In particular, if &amp;lt;math&amp;gt;\mathcal{P}&amp;lt;/math&amp;gt; is initially on the space-fixed &#039;&#039;Z&#039;&#039;-axis, it has&lt;br /&gt;
the space-fixed coordinates&lt;br /&gt;
:&amp;lt;math&amp;gt; &lt;br /&gt;
\mathbf{R}(\alpha,\beta,\gamma)&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
0 \\&lt;br /&gt;
0 \\&lt;br /&gt;
r \\&lt;br /&gt;
\end{pmatrix}=&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
r \cos\alpha\sin\beta \\&lt;br /&gt;
r \sin\alpha \sin\beta \\&lt;br /&gt;
r \cos\beta \\&lt;br /&gt;
\end{pmatrix},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
which shows the correspondence with the [[Spherical coordinate system|spherical polar coordinates]] &lt;br /&gt;
(in the physical convention).&lt;br /&gt;
&lt;br /&gt;
Knowledge of the Euler angles as function of time &#039;&#039;t&#039;&#039; and the initial coordinates &amp;lt;math&amp;gt;\mathbf{r}(0)&amp;lt;/math&amp;gt;  determine the kinematics of the rigid rotor.&lt;br /&gt;
&lt;br /&gt;
=== Classical kinetic energy ===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;small&amp;gt; The following text forms a generalization of the well-known special case of the [[rotational energy]] of an object that rotates around &#039;&#039;one&#039;&#039; axis.&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It will be assumed from here on that the body-fixed frame is a principal axes frame; it diagonalizes the instantaneous [[moment of inertia tensor|inertia tensor]] &amp;lt;math&amp;gt; \mathbf{I}(t)&amp;lt;/math&amp;gt; (expressed with respect to the space-fixed frame), i.e.,&lt;br /&gt;
:&amp;lt;math&amp;gt; &lt;br /&gt;
\mathbf{R}(\alpha,\beta,\gamma)^{-1}\; \mathbf{I}(t)\; \mathbf{R}(\alpha,\beta,\gamma)&lt;br /&gt;
= \mathbf{I}(0)\quad\hbox{with}\quad&lt;br /&gt;
\mathbf{I}(0) =&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
I_1 &amp;amp; 0 &amp;amp; 0 \\ 0 &amp;amp; I_2 &amp;amp; 0 \\ 0 &amp;amp; 0 &amp;amp; I_3 \\&lt;br /&gt;
\end{pmatrix},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where the Euler angles are time-dependent and in fact determine the time dependence of &amp;lt;math&amp;gt;\mathbf{I}(t)&amp;lt;/math&amp;gt; by the inverse of this equation. This notation implies&lt;br /&gt;
that at &amp;lt;math&amp;gt;t=0&amp;lt;/math&amp;gt; the Euler angles are zero, so that at &amp;lt;math&amp;gt;t=0&amp;lt;/math&amp;gt; the body-fixed frame coincides with the space-fixed frame.&lt;br /&gt;
&lt;br /&gt;
The classical kinetic energy &#039;&#039;T&#039;&#039;  of the rigid rotor can be expressed in different ways:&lt;br /&gt;
* as a function  of angular velocity&lt;br /&gt;
* in Lagrangian form&lt;br /&gt;
* as a function of angular momentum&lt;br /&gt;
* in Hamiltonian form.&lt;br /&gt;
&lt;br /&gt;
Since each of these forms has its use and can be found in textbooks we will present all of them.&lt;br /&gt;
&lt;br /&gt;
==== Angular velocity form ====&lt;br /&gt;
&lt;br /&gt;
As a function of angular velocity &#039;&#039;T&#039;&#039; reads,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
 T = \frac{1}{2} \left[ I_1 \omega_x^2 + I_2 \omega_y^2+ I_3 \omega_z^2 \right]&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
with&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\omega_x \\&lt;br /&gt;
\omega_y \\&lt;br /&gt;
\omega_z \\&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
= &lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
-\sin\beta\cos\gamma &amp;amp; \sin\gamma &amp;amp; 0 \\&lt;br /&gt;
 \sin\beta\sin\gamma &amp;amp; \cos\gamma &amp;amp; 0 \\&lt;br /&gt;
    \cos\beta        &amp;amp;        0   &amp;amp; 1 \\&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\dot{\alpha} \\&lt;br /&gt;
\dot{\beta} \\&lt;br /&gt;
\dot{\gamma} \\&lt;br /&gt;
\end{pmatrix}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
The  vector &amp;lt;math&amp;gt;\boldsymbol{\omega} = (\omega_x, \omega_y, \omega_z) &amp;lt;/math&amp;gt; contains the components of the [[angular velocity]] of the rotor expressed with respect to the body-fixed frame. It can be shown that &amp;lt;math&amp;gt;\boldsymbol{\omega}&amp;lt;/math&amp;gt; is &#039;&#039;not&#039;&#039; the time derivative of any vector, in contrast to the usual [[Velocity#Formal description|definition of velocity]].&amp;lt;ref name=&amp;quot;Goldstein&amp;quot;&amp;gt;Chapter 4.9 of Goldstein, H.; Poole, C. P.; Safko, J. L. (2001). Classical Mechanics (Third ed.). San Francisco: Addison Wesley Publishing Company. ISBN 0-201-65702-3.&amp;lt;/ref&amp;gt; The dots over the time-dependent Euler angles indicate [[Newton&#039;s notation for differentiation|time derivatives]].&lt;br /&gt;
The angular velocity satisfies  equations of motion known as [[Euler&#039;s equations]] (with zero applied torque, since by assumption the rotor is in field-free space).&lt;br /&gt;
&lt;br /&gt;
==== Lagrange form ====&lt;br /&gt;
&lt;br /&gt;
Backsubstitution of the expression of  &amp;lt;math&amp;gt;\boldsymbol{\omega}&amp;lt;/math&amp;gt; into &#039;&#039;T&#039;&#039; gives&lt;br /&gt;
the kinetic energy in [[Lagrangian mechanics|Lagrange form]] (as a function of the time derivatives of the Euler angles). In matrix-vector notation,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
2 T =&lt;br /&gt;
\begin{pmatrix} &lt;br /&gt;
\dot{\alpha} &amp;amp; \dot{\beta} &amp;amp; \dot{\gamma}&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
\; \mathbf{g} \;&lt;br /&gt;
\begin{pmatrix} &lt;br /&gt;
\dot{\alpha} \\ \dot{\beta} \\ \dot{\gamma}\\&lt;br /&gt;
\end{pmatrix},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\mathbf{g}&amp;lt;/math&amp;gt; is the metric tensor expressed in Euler angles&amp;amp;mdash;a non-orthogonal system of [[curvilinear coordinates]]&amp;amp;mdash;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\mathbf{g}=&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
I_1 \sin^2\beta \cos^2\gamma+I_2\sin^2\beta\sin^2\gamma+I_3\cos^2\beta &amp;amp;&lt;br /&gt;
(I_2-I_1) \sin\beta\sin\gamma\cos\gamma &amp;amp;&lt;br /&gt;
I_3\cos\beta \\&lt;br /&gt;
(I_2-I_1) \sin\beta\sin\gamma\cos\gamma &amp;amp;&lt;br /&gt;
I_1\sin^2\gamma+I_2\cos^2\gamma &amp;amp; 0 \\&lt;br /&gt;
I_3\cos\beta &amp;amp; 0 &amp;amp; I_3 \\&lt;br /&gt;
\end{pmatrix}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Angular momentum form ====&lt;br /&gt;
&lt;br /&gt;
Often the kinetic energy is written as a function of the [[Angular momentum#Angular momentum in classical mechanics|angular momentum]] &amp;lt;math&amp;gt;\vec{L}&amp;lt;/math&amp;gt; of the rigid rotor. This vector is a conserved (time-independent) quantity.&lt;br /&gt;
With respect to the  body-fixed frame it has the components &amp;lt;math&amp;gt;\mathbf{L}&amp;lt;/math&amp;gt;, which can be shown to &lt;br /&gt;
be related to the angular velocity,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\mathbf{L} = &lt;br /&gt;
\mathbf{I}(0)\;&lt;br /&gt;
\boldsymbol{\omega}\quad\hbox{or}\quad L_i = \frac{\partial T}{\partial\omega_i},\;\; i=x,\,y,\,z.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
Since the body-fixed frame moves (depends on time) these components are &#039;&#039;not&#039;&#039; time independent. If we were&lt;br /&gt;
to represent &amp;lt;math&amp;gt;\vec{L}&amp;lt;/math&amp;gt; with respect to the stationary space-fixed frame, we would&lt;br /&gt;
find time independent expressions for its components.&lt;br /&gt;
The kinetic energy is given by &lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
 T = \frac{1}{2} \left[ \frac{L_x^2}{I_1} + \frac{L_y^2}{I_2}+ \frac{L_z^2}{I_3}\right].&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==== Hamilton form ====&lt;br /&gt;
&lt;br /&gt;
The  [[Hamiltonian mechanics|Hamilton form]] of the kinetic energy is written in terms&lt;br /&gt;
of generalized momenta&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
p_\alpha \\&lt;br /&gt;
p_\beta \\&lt;br /&gt;
p_\gamma \\&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
\ \stackrel{\mathrm{def}}{=}\  &lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\partial T/{\partial \dot{\alpha}}\\ &lt;br /&gt;
\partial T/{\partial \dot{\beta}} \\&lt;br /&gt;
\partial T/{\partial \dot{\gamma}} \\&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
= \mathbf{g} &lt;br /&gt;
\begin{pmatrix} \; \,&lt;br /&gt;
\dot{\alpha} \\ \dot{\beta} \\ \dot{\gamma}\\&lt;br /&gt;
\end{pmatrix},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where it is used that the &amp;lt;math&amp;gt;\mathbf{g}&amp;lt;/math&amp;gt; is symmetric.&lt;br /&gt;
In Hamilton form the kinetic energy is,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
2 T =&lt;br /&gt;
\begin{pmatrix} &lt;br /&gt;
p_{\alpha} &amp;amp; p_{\beta} &amp;amp; p_{\gamma}&lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
\; \mathbf{g}^{-1} \;&lt;br /&gt;
\begin{pmatrix} &lt;br /&gt;
p_{\alpha} \\ p_{\beta} \\ p_{\gamma}\\&lt;br /&gt;
\end{pmatrix},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
with the inverse metric tensor given by&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
{\scriptstyle \sin^2\beta}\;\;\mathbf{g}^{-1}= &lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
\frac{\cos^2\gamma}{I_1}+\frac{\sin^2\gamma}{I_2} &amp;amp;&lt;br /&gt;
\left(\frac{1}{I_2}-\frac{1}{I_1}\right){\scriptstyle \sin\beta\sin\gamma\cos\gamma}&amp;amp;&lt;br /&gt;
-\frac{\cos\beta\cos^2\gamma}{I_1}-\frac{\cos\beta\sin^2\gamma}{I_2} \\&lt;br /&gt;
\left(\frac{1}{I_2}-\frac{1}{I_1}\right){\scriptstyle \sin\beta\sin\gamma\cos\gamma}&amp;amp;&lt;br /&gt;
\frac{\sin^2\beta\sin^2\gamma}{I_1}+\frac{\sin^2\beta\cos^2\gamma}{I_2} &amp;amp;&lt;br /&gt;
\left(\frac{1}{I_1}-\frac{1}{I_2}\right){\scriptstyle \sin\beta\cos\beta\sin\gamma\cos\gamma}\\&lt;br /&gt;
-\frac{\cos\beta\cos^2\gamma}{I_1}-\frac{\cos\beta\sin^2\gamma}{I_2} &amp;amp;&lt;br /&gt;
\left(\frac{1}{I_1}-\frac{1}{I_2}\right){\scriptstyle \sin\beta\cos\beta\sin\gamma\cos\gamma} &amp;amp;&lt;br /&gt;
\frac{\cos^2\beta\cos^2\gamma}{I_1}+ \frac{\cos^2\beta\sin^2\gamma}{I_2}+\frac{\sin^2\beta}{I_3} \\&lt;br /&gt;
\end{pmatrix}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
This inverse tensor is needed to obtain the [[Laplace-Beltrami operator]], which (multiplied&lt;br /&gt;
by &amp;lt;math&amp;gt;-\hbar^2&amp;lt;/math&amp;gt;) gives the quantum mechanical energy operator&lt;br /&gt;
of the rigid rotor.&lt;br /&gt;
&lt;br /&gt;
The classical Hamiltonian given above can be rewritten to the following expression, which is needed in the phase integral&lt;br /&gt;
arising in the classical statistical mechanics of rigid rotors,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{array}{lcl}&lt;br /&gt;
T &amp;amp;=&amp;amp; \frac{1}{2I_1 \sin^2\beta}&lt;br /&gt;
    \left( (p_\alpha- p_\gamma\cos\beta)\cos\gamma -p_\beta&lt;br /&gt;
        \sin\beta\sin\gamma \right)^2  \\&lt;br /&gt;
  &amp;amp;&amp;amp;+ \frac{1}{2I_2 \sin^2\beta}&lt;br /&gt;
    \left( (p_\alpha- p_\gamma\cos\beta)\sin\gamma +p_\beta&lt;br /&gt;
     \sin\beta\cos\gamma \right)^2 + \frac{p_\gamma^2}{2I_3}.  \\&lt;br /&gt;
\end{array}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Quantum mechanical rigid rotor ===&lt;br /&gt;
{{see also|Rotational spectroscopy}}&lt;br /&gt;
As usual quantization is performed by the replacement of the generalized momenta&lt;br /&gt;
by operators that give first derivatives with respect to its [[Canonically conjugate coordinates|canonically conjugate]] variables (positions). Thus,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
p_\alpha \longrightarrow -i \hbar \frac{\partial}{\partial \alpha}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
and similarly for &amp;lt;math&amp;gt;p_\beta&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;p_\gamma&amp;lt;/math&amp;gt;. It is remarkable that this rule replaces the fairly complicated function &amp;lt;math&amp;gt;p_\alpha&amp;lt;/math&amp;gt; of all three Euler angles, time derivatives of Euler angles, and inertia moments (characterizing the rigid rotor) by a simple differential operator that  does not depend on time or inertia moments and differentiates to one Euler angle only. &lt;br /&gt;
&lt;br /&gt;
The quantization rule is sufficient to obtain the operators&lt;br /&gt;
that correspond with the classical angular momenta. There are two kinds: space-fixed and body-fixed&lt;br /&gt;
angular momentum operators. Both are vector operators, i.e., both have three components&lt;br /&gt;
that transform as vector components among themselves upon rotation of the space-fixed and  the body-fixed frame, respectively. The explicit form of the rigid rotor angular momentum operators is&lt;br /&gt;
given [[Wigner D-matrix|here]] (but beware, they must be multiplied with &amp;lt;math&amp;gt;\hbar&amp;lt;/math&amp;gt;). The body-fixed angular momentum operators are written&lt;br /&gt;
as &amp;lt;math&amp;gt;\hat{\mathcal{P}}_i&amp;lt;/math&amp;gt;. They satisfy [[Wigner D-matrix#Properties of Wigner D-matrix|&#039;&#039;anomalous commutation relations&#039;&#039;]].&lt;br /&gt;
&lt;br /&gt;
The quantization rule is &#039;&#039;not&#039;&#039; sufficient to obtain the kinetic energy operator from&lt;br /&gt;
the classical Hamiltonian. Since classically &amp;lt;math&amp;gt;p_\beta&amp;lt;/math&amp;gt; commutes with &amp;lt;math&amp;gt;\cos\beta&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\sin\beta&amp;lt;/math&amp;gt; and the inverses of these functions, the position&lt;br /&gt;
of these trigonometric functions in the classical Hamiltonian is arbitrary. After&lt;br /&gt;
quantization the commutation does no longer hold and the order of operators and functions in the Hamiltonian (energy operator) becomes a point of concern. Podolsky&amp;lt;ref name=&amp;quot;Podolsky&amp;quot; /&amp;gt; proposed in 1928 that the [[Laplace-Beltrami operator#Laplace–Beltrami operator|Laplace-Beltrami operator]]&lt;br /&gt;
(times &amp;lt;math&amp;gt;-\tfrac{1}{2}\hbar^2&amp;lt;/math&amp;gt;) has the appropriate  form for the quantum mechanical kinetic &lt;br /&gt;
energy operator. This operator has the general  form (summation convention: sum over repeated indices&amp;amp;mdash;in this case over the three Euler angles &amp;lt;math&amp;gt; q^1,\,q^2,\,q^3 \equiv \alpha,\,\beta,\,\gamma&amp;lt;/math&amp;gt;):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{H} = - \tfrac{\hbar^2}{2}\;|g|^{-1/2}&lt;br /&gt;
\frac{\partial}{\partial q^i} |g|^{1/2} g^{ij} \frac{\partial}{\partial q^j},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;|g|&amp;lt;/math&amp;gt; is the determinant of the g-tensor:&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
|g| = I_1\, I_2\, I_3\, \sin^2 \beta \quad \hbox{and}\quad g^{ij} = (\mathbf{g}^{-1})_{ij}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
Given the inverse of the metric tensor above, the explicit form of the kinetic energy operator in terms of Euler angles follows by simple substitution. (Note: The corresponding eigenvalue equation&lt;br /&gt;
gives the [[Schrödinger equation]] for the rigid rotor in the form that it was&lt;br /&gt;
solved for the first time by Kronig and Rabi&amp;lt;ref name=&amp;quot;Kronig&amp;quot;&amp;gt;{{cite journal| doi=10.1103/PhysRev.29.262| author=R. de L. Kronig and I. I. Rabi| title=The Symmetrical Top in the Undulatory Mechanics|journal= Phys. Rev.|volume= 29|pages= 262–269 |year=1927|bibcode = 1927PhRv...29..262K }}&amp;lt;/ref&amp;gt; (for the special case of the symmetric rotor). This is one of the few cases where the Schrödinger equation can be solved analytically. All these cases were solved within a year of the formulation of the Schrödinger equation.)&lt;br /&gt;
&lt;br /&gt;
Nowadays it is  common to proceed as follows. It can be shown that &amp;lt;math&amp;gt;\hat{H}&amp;lt;/math&amp;gt;&lt;br /&gt;
can be expressed in body-fixed angular momentum operators (in this proof one must carefully&lt;br /&gt;
commute differential operators with trigonometric functions). The result has the same appearance&lt;br /&gt;
as the classical formula expressed in body-fixed coordinates,&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{H} = \tfrac{1}{2}\left[ \frac{\mathcal{P}_x^2}{I_1}+ \frac{\mathcal{P}_y^2}{I_2}+&lt;br /&gt;
\frac{\mathcal{P}_z^2}{I_3} \right].&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
The action of the &amp;lt;math&amp;gt;\hat{\mathcal{P}}_i&amp;lt;/math&amp;gt; on the [[Wigner D-matrix#Properties of Wigner D-matrix|Wigner D-matrix]] is simple. In particular&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\mathcal{P}^2\, D^j_{m&#039;m}(\alpha,\beta,\gamma)^* = \hbar^2 j(j+1) D^j_{m&#039;m}(\alpha,\beta,\gamma)^* \quad\hbox{with}\quad&lt;br /&gt;
\mathcal{P}^2= \mathcal{P}^2_x + \mathcal{P}_y^2+ \mathcal{P}_z^2,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
so that the Schrödinger  equation for the spherical rotor (&amp;lt;math&amp;gt;I=I_1=I_2=I_3&amp;lt;/math&amp;gt;)  &lt;br /&gt;
is solved with the &amp;lt;math&amp;gt; (2j+1)^2 &amp;lt;/math&amp;gt; degenerate energy equal to &amp;lt;math&amp;gt;\tfrac{\hbar^2 j(j+1)}{2I}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The symmetric top (= symmetric rotor) is characterized by &amp;lt;math&amp;gt;I_1=I_2&amp;lt;/math&amp;gt;. It is &lt;br /&gt;
a &#039;&#039;prolate&#039;&#039; (cigar shaped) top if &amp;lt;math&amp;gt;I_3 &amp;lt; I_1=I_2 &amp;lt;/math&amp;gt;. In the latter&lt;br /&gt;
case we write the Hamiltonian as&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{H} = \tfrac{1}{2}\left[ \frac{\mathcal{P}^2}{I_1}+ \mathcal{P}_z^2\Big(\frac{1}{I_3}&lt;br /&gt;
-\frac{1}{I_1} \Big) \right],&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
and use that &lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\mathcal{P}_z^2\, D^j_{m k}(\alpha,\beta,\gamma)^* = \hbar^2 k^2\, D^j_{m k}(\alpha,\beta,\gamma)^*.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
Hence&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{H}\,D^j_{m k}(\alpha,\beta,\gamma)^* = E_{jk} D^j_{m k}(\alpha,\beta,\gamma)^*&lt;br /&gt;
\quad \hbox{with}\quad E_{jk}/ \hbar^2 = \frac{j(j+1)}{2I_1} + k^2\left(\frac{1}{2I_3}-\frac{1}{2I_1}\right).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
The eigenvalue &amp;lt;math&amp;gt;E_{j0}&amp;lt;/math&amp;gt; is &amp;lt;math&amp;gt;2j+1&amp;lt;/math&amp;gt;-fold degenerate, for all eigenfunctions&lt;br /&gt;
with &amp;lt;math&amp;gt;m=-j,-j+1,\dots, j &amp;lt;/math&amp;gt; have the same eigenvalue.  The energies with |k| &amp;gt; 0 are&lt;br /&gt;
&amp;lt;math&amp;gt;2(2j+1)&amp;lt;/math&amp;gt;-fold degenerate. This exact solution of the&lt;br /&gt;
Schrödinger equation of the symmetric top was first found in 1927.&amp;lt;ref name=&amp;quot;Kronig&amp;quot; /&amp;gt; &lt;br /&gt;
&lt;br /&gt;
The asymmetric top problem (&amp;lt;math&amp;gt; I_1 \ne I_2 \ne I_3 &amp;lt;/math&amp;gt;) is not exactly soluble.&lt;br /&gt;
&lt;br /&gt;
==Direct experimental observation of molecular rotations==&lt;br /&gt;
&lt;br /&gt;
For long time, molecular rotations could not be directly observed experimentally. Only measurement techniques with atomic resolution made it possible to detect the rotation of a single molecule.&amp;lt;ref&amp;gt;{{Literatur | Autor = J. K. Gimzewski, C. Joachim, R. R. Schlittler, V. Langlais, H. Tang, I. Johannsen | Titel = Rotation of a Single Molecule Within a Supramolecular Bearing | Sammelwerk = Science | Band = 281 | Jahr = 1998 | Datum = 1998-07-24| Nummer = 5376| Seiten = 531–533| DOI= 10.1126/science.281.5376.531}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;ReferenceA&amp;quot;&amp;gt;{{Literatur | Autor = Thomas Waldmann, Jens Klein, Harry E. Hoster, R. Jürgen Behm | Titel = Stabilization of Large Adsorbates by Rotational Entropy: A Time-Resolved Variable-Temperature STM Study | Sammelwerk = ChemPhysChem | Jahr = 2012 | Datum = 2012| Seiten = n/a–n/a| DOI= 10.1002/cphc.201200531}}&amp;lt;/ref&amp;gt; At low temperatures, the rotations of molecules (or part thereof) can be frozen. This could be directly visualized by [[Scanning tunneling microscope|Scanning tunneling microscopy]] i.e., the stabilization could be explained at higher temperatures the rotational entropy.&amp;lt;ref name=&amp;quot;ReferenceA&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Balancing machine]]&lt;br /&gt;
*[[Gyroscope]]&lt;br /&gt;
*[[Infrared spectroscopy]]&lt;br /&gt;
*[[Rigid body]]&lt;br /&gt;
*[[Rotational spectroscopy]]&lt;br /&gt;
*[[Spectroscopy]]&lt;br /&gt;
*[[Vibrational spectroscopy]]&lt;br /&gt;
*[[Quantum rotor model]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;!-- ----------------------------------------------------------&lt;br /&gt;
  See http://en.wikipedia.org/wiki/Wikipedia:Footnotes for a &lt;br /&gt;
  discussion of different citation methods and how to generate &lt;br /&gt;
  footnotes using the&amp;amp;lt;ref&amp;gt;, &amp;amp;lt;/ref&amp;gt; and  &amp;amp;lt;reference /&amp;gt; tags&lt;br /&gt;
----------------------------------------------------------- --&amp;gt;&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
==General references==&lt;br /&gt;
* {{cite journal|doi=10.1103/RevModPhys.3.280|author=D. M. Dennison|title=The Infrared Spectra of Polyatomic Molecules Part I|journal= Rev. Mod. Physics|volume=3|pages=280–345|year=1931|bibcode = 1931RvMP....3..280D }} (Especially Section 2: The Rotation of Polyatomic Molecules).&lt;br /&gt;
* {{Cite journal| doi=10.1103/RevModPhys.23.213| first=J. H.|last= Van Vleck| title=The Coupling of Angular Momentum Vectors in Molecules|journal= Rev. Mod. Physics| volume=23|pages=213–227 |year=1951|bibcode = 1951RvMP...23..213V }}&lt;br /&gt;
* {{cite book | author=McQuarrie, Donald A | title=Quantum Chemistry | location=Mill Valley, Calif.  | publisher=University Science Books | year=1983 | isbn=0-935702-13-X}}&lt;br /&gt;
* {{cite book| isbn= 0-201-65702-3| first1= H. |last1=Goldstein|first2=C. P. |last2=Poole|first3= J. L.|last3= Safko| title=Classical Mechanics|edition=Third |publisher= Addison Wesley Publishing Company|location= San Francisco |year=2001}} (Chapters 4 and 5)&lt;br /&gt;
*  {{cite book| isbn=0-387-96890-3| first= V. I.|last= Arnold|title=Mathematical Methods of Classical Mechanics|publisher= Springer-Verlag |year=1989}} (Chapter 6).&lt;br /&gt;
* {{cite book| first=H. W. |last=Kroto| title=Molecular Rotation Spectra|publisher= Dover |location=New York|year=1992}}&lt;br /&gt;
* {{cite book|first1=W.|last1= Gordy |first2= R. L. |last2=Cook|title=Microwave Molecular Spectra|edition=Third| publisher=Wiley|location= New York |year=1984|isbn=0-471-08681-9}}&lt;br /&gt;
* {{cite book| first1=D. |last1=Papoušek |first2= M. T. |last2=Aliev|title=Molecular Vibrational-Rotational Spectra|publisher=Elsevier|location= Amsterdam |year=1982| isbn=0-444-99737-7}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Molecular physics]]&lt;br /&gt;
[[Category:Rigid bodies]]&lt;br /&gt;
[[Category:Rotation]]&lt;/div&gt;</summary>
		<author><name>131.111.24.210</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Electric_displacement_field&amp;diff=7842</id>
		<title>Electric displacement field</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Electric_displacement_field&amp;diff=7842"/>
		<updated>2014-01-21T23:00:08Z</updated>

		<summary type="html">&lt;p&gt;131.111.216.174: /* Example: Displacement field in a capacitor */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:Zurich sunspot number since 1750.png|thumb|350px|Wolf number since 1750.]]&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;&#039;Wolf number&#039;&#039;&#039; (also known as the &#039;&#039;&#039;International sunspot number&#039;&#039;&#039;, &#039;&#039;&#039;relative sunspot number&#039;&#039;&#039;, or &#039;&#039;&#039;Zürich number&#039;&#039;&#039;) is a quantity that measures the number of [[sunspots]] and groups of sunspots present on the surface of the sun.&lt;br /&gt;
&lt;br /&gt;
The idea of computing sunspot numbers was originated by [[Rudolf Wolf]] in 1848&amp;lt;ref&amp;gt;{{cite web|title=The Sun - History|url=http://www-istp.gsfc.nasa.gov/Education/whsun.html|date=2001-11-25|accessdate=2012-01-08}}&amp;lt;/ref&amp;gt; in [[Zurich]], [[Switzerland]] and, thus, the procedure he initiated bears his name (or place). The combination of sunspots and their grouping is used because it compensates for variations in observing small sunspots.&lt;br /&gt;
&lt;br /&gt;
This number has been collected and tabulated by researchers for over 150 years. They have found that sunspot activity is cyclical and reaches its maximum around every 9.5 to 11 years (note: Using data from [http://sidc.oma.be/ SIDC] for the last 300 years and running a [[Discrete Fourier transform|FFT]] function on the data gives an average maximum at 10.4883 years/cycle).&amp;lt;ref&amp;gt;[http://sidc.oma.be/ SIDC], RWC Belgium, World Data Center for the Sunspot Index, [[Observatoire Royal de Belgique|Royal Observatory of Belgium]], &#039;year(s)-of-data&#039;.&amp;lt;/ref&amp;gt; This cycle was first noted by [[Heinrich Schwabe]] in 1843.&lt;br /&gt;
&lt;br /&gt;
The relative sunspot number &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt; is computed using the formula (collected as a daily index of sunspot activity):&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;R = k(10g + s) \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
&lt;br /&gt;
* &amp;lt;math&amp;gt;s&amp;lt;/math&amp;gt; is the number of individual spots,&lt;br /&gt;
* &amp;lt;math&amp;gt;g&amp;lt;/math&amp;gt; is the number of sunspot groups, and&lt;br /&gt;
* &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt; is a factor that varies with location and instrumentation (also known as the &#039;&#039;observatory factor&#039;&#039; or the &#039;&#039;personal reduction coefficient&#039;&#039; &amp;lt;math&amp;gt;K&amp;lt;/math&amp;gt;).&amp;lt;ref&amp;gt;[http://www.sidc.be/news/106/sunspotnumberclarified.pdf personal reduction coefficient K]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Solar variation]]&lt;br /&gt;
* [[Joy&#039;s Law (astronomy)]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [http://cse.ssl.berkeley.edu/segwayed/lessons/sunspots/ The Exploratorium&#039;s Guide to Sunspots]&lt;br /&gt;
* [http://sidc.oma.be/index.php3 RWC Belgium World Data Center for the Sunspot Index]&lt;br /&gt;
* [http://solarscience.msfc.nasa.gov/SunspotCycle.shtml NASA Solar Physics Sunspot Cycle page] and [http://solarscience.msfc.nasa.gov/greenwch/spot_num.txt Table of Sunspot Numbers (txt)] by month since 1749 CE&lt;br /&gt;
&lt;br /&gt;
{{The Sun}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Stellar phenomena]]&lt;br /&gt;
[[Category:Solar phenomena]]&lt;br /&gt;
&lt;br /&gt;
[[de:Sonnenfleck#Sonnenflecken-Relativzahl]]&lt;/div&gt;</summary>
		<author><name>131.111.216.174</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Max%E2%80%93min_inequality&amp;diff=26856</id>
		<title>Max–min inequality</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Max%E2%80%93min_inequality&amp;diff=26856"/>
		<updated>2014-01-20T09:53:34Z</updated>

		<summary type="html">&lt;p&gt;131.111.20.56: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[abstract algebra]], specifically in [[module theory]], a &#039;&#039;&#039;dense submodule&#039;&#039;&#039; of a module is a refinement of the notion of an [[essential submodule]].  If &#039;&#039;N&#039;&#039; is a dense submodule of &#039;&#039;M&#039;&#039;, it may also be said it may alternatively be said that &amp;quot;&#039;&#039;N&#039;&#039;&amp;amp;nbsp;⊆&amp;amp;nbsp;&#039;&#039;M&#039;&#039; is a &#039;&#039;&#039;rational extension&#039;&#039;&#039;&amp;quot;. Dense submodules are connected with rings of quotients in noncommutative ring theory. Most of the results appearing here were first established in {{harv|Johnson|1951}}, {{harv|Utumi|1956}} and {{harv|Findlay|Lambek|1958}}.&lt;br /&gt;
&lt;br /&gt;
It should be noticed that this terminology is different from the notion of a [[dense subset]] in [[general topology]].  No topology is needed to define a dense submodule, and a dense submodule may or may not be topologically dense in a module with topology.&lt;br /&gt;
&lt;br /&gt;
== Definition ==&lt;br /&gt;
This article modifies [[Exposition (literary technique)|exposition]] appearing in {{harv|Storrer|1972}} and {{harv|Lam|1999|p=272}}. Let &#039;&#039;R&#039;&#039; be a ring, and &#039;&#039;M&#039;&#039; be a right &#039;&#039;R&#039;&#039; module with submodule &#039;&#039;N&#039;&#039;.  For an element &#039;&#039;y&#039;&#039; of &#039;&#039;M&#039;&#039;, define&lt;br /&gt;
:&amp;lt;math&amp;gt;y^{-1}N=\{r\in R \mid yr\in N \} \,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Note that the expression &#039;&#039;y&#039;&#039;&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt; is only formal and that &#039;&#039;y&#039;&#039; is not necessarily [[invertible]], but it helps to suggest that &#039;&#039;y&#039;&#039;⋅(&#039;&#039;y&#039;&#039;&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;&#039;&#039;N&#039;&#039;)&amp;amp;nbsp;⊆&amp;amp;nbsp;&#039;&#039;N&#039;&#039;. The set &#039;&#039;y&#039;&#039;&amp;amp;nbsp;&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;&#039;&#039;N&#039;&#039; is always a right [[ideal (ring theory)|ideal]] of &#039;&#039;R&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
A submodule &#039;&#039;N&#039;&#039; of &#039;&#039;M&#039;&#039; is said to be a &#039;&#039;&#039;dense submodule&#039;&#039;&#039; if for all &#039;&#039;x&#039;&#039; and &#039;&#039;y&#039;&#039; in &#039;&#039;M&#039;&#039; with &#039;&#039;x&#039;&#039;&amp;amp;nbsp;≠&amp;amp;nbsp;0, there exists an &#039;&#039;r&#039;&#039; in &#039;&#039;R&#039;&#039; such that &#039;&#039;xr&#039;&#039;&amp;amp;nbsp;≠&amp;amp;nbsp;{0} and &#039;&#039;yr&#039;&#039; is in &#039;&#039;N&#039;&#039;.  In other words, using the introduced notation, the set&lt;br /&gt;
:&amp;lt;math&amp;gt;x(y^{-1}N)\neq\{0\} \,&amp;lt;/math&amp;gt;&lt;br /&gt;
In this case, the relationship is denoted by&lt;br /&gt;
:&amp;lt;math&amp;gt;N\subseteq_d M\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Another equivalent definition is [[homological algebra|homological]] in nature: &#039;&#039;N&#039;&#039; is dense in &#039;&#039;M&#039;&#039; if and only if&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathrm{Hom}_R (M/N,E(M))=\{0\}\,&amp;lt;/math&amp;gt;&lt;br /&gt;
where &#039;&#039;E&#039;&#039;(&#039;&#039;M&#039;&#039;) is the [[injective hull]] of &#039;&#039;M&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
== Properties ==&lt;br /&gt;
* It can be shown that &#039;&#039;N&#039;&#039; is an essential submodule of &#039;&#039;M&#039;&#039; if and only if for all &#039;&#039;y&#039;&#039;&amp;amp;nbsp;≠&amp;amp;nbsp;0 in &#039;&#039;M&#039;&#039;, the set &#039;&#039;y&#039;&#039;⋅(&#039;&#039;y&#039;&#039;&amp;amp;nbsp;&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;&#039;&#039;N&#039;&#039;)&amp;amp;nbsp;≠&amp;amp;nbsp;{0}.  Clearly then, every dense submodule is an essential submodule.&lt;br /&gt;
* If &#039;&#039;M&#039;&#039; is a [[nonsingular module]], then &#039;&#039;N&#039;&#039; is dense in &#039;&#039;M&#039;&#039; if and only if it is essential in &#039;&#039;M&#039;&#039;.&lt;br /&gt;
* A ring is a right [[nonsingular ring]] if and only if its essential right ideals are all dense right ideals.&lt;br /&gt;
* If &#039;&#039;N&#039;&#039; and &#039;&#039;N&#039; &#039;&#039; are dense submodules of &#039;&#039;M&#039;&#039;, then so is &#039;&#039;N&#039;&#039;&amp;amp;nbsp;∩&amp;amp;nbsp;&#039;&#039;N&#039; &#039;&#039;.&lt;br /&gt;
* If &#039;&#039;N&#039;&#039; is dense and &#039;&#039;N&#039;&#039;&amp;amp;nbsp;⊆&amp;amp;nbsp;&#039;&#039;K&#039;&#039;&amp;amp;nbsp;⊆&amp;amp;nbsp;&#039;&#039;M&#039;&#039;, then &#039;&#039;K&#039;&#039; is also dense.&lt;br /&gt;
* If &#039;&#039;B&#039;&#039; is a dense right ideal in &#039;&#039;R&#039;&#039;, then so is &#039;&#039;y&#039;&#039;&amp;lt;sup&amp;gt;−1&amp;lt;/sup&amp;gt;&#039;&#039;B&#039;&#039; for any &#039;&#039;y&#039;&#039; in &#039;&#039;R&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
== Examples ==&lt;br /&gt;
* If &#039;&#039;x&#039;&#039; is a non-zerodivisor in the [[center (algebra)|center]] of &#039;&#039;R&#039;&#039;, then &#039;&#039;xR&#039;&#039; is a dense right ideal of &#039;&#039;R&#039;&#039;.&lt;br /&gt;
* If &#039;&#039;I&#039;&#039; is a two-sided ideal of &#039;&#039;R&#039;&#039;, &#039;&#039;I&#039;&#039; is dense as a right ideal if and only if the &#039;&#039;left&#039;&#039; [[annihilator]] of &#039;&#039;I&#039;&#039; is zero, that is, &amp;lt;math&amp;gt;\ell\cdot \mathrm{Ann}(I)=\{0\}\,&amp;lt;/math&amp;gt;.  In particular in commutative rings, the dense ideals are precisely the ideals which are [[faithful module]]s.&lt;br /&gt;
&lt;br /&gt;
== Applications ==&lt;br /&gt;
=== Rational hull of a module ===&lt;br /&gt;
Every right &#039;&#039;R&#039;&#039; module &#039;&#039;M&#039;&#039; has a maximal essential extension &#039;&#039;E&#039;&#039;(&#039;&#039;M&#039;&#039;) which is its [[injective hull]].  The analogous construction using a maximal dense extension results in the &#039;&#039;&#039;rational hull&#039;&#039;&#039; &#039;&#039;Ẽ&#039;&#039;(&#039;&#039;M&#039;&#039;) which is a submodule of &#039;&#039;E&#039;&#039;(&#039;&#039;M&#039;&#039;).  When a module has no proper rational extension, so that &#039;&#039;Ẽ&#039;&#039;(&#039;&#039;M&#039;&#039;)&amp;amp;nbsp;=&amp;amp;nbsp;&#039;&#039;M&#039;&#039;, the module is said to be &#039;&#039;&#039;rationally complete&#039;&#039;&#039;.  If &#039;&#039;R&#039;&#039; is right nonsingular, then of course &#039;&#039;Ẽ&#039;&#039;(&#039;&#039;M&#039;&#039;)&amp;amp;nbsp;=&amp;amp;nbsp;&#039;&#039;E&#039;&#039;(&#039;&#039;M&#039;&#039;).&lt;br /&gt;
&lt;br /&gt;
The rational hull is readily identified within the injective hull.  Let &#039;&#039;S&#039;&#039;=End&amp;lt;sub&amp;gt;&#039;&#039;R&#039;&#039;&amp;lt;/sub&amp;gt;(&#039;&#039;E&#039;&#039;(&#039;&#039;M&#039;&#039;)) be the [[endomorphism ring]] of the injective hull.  Then an element &#039;&#039;x&#039;&#039; of the injective hull is in the rational hull if and only if &#039;&#039;x&#039;&#039; is sent to zero by all maps in &#039;&#039;S&#039;&#039; which are zero on &#039;&#039;M&#039;&#039;.  In symbols,&lt;br /&gt;
:&amp;lt;math&amp;gt;\tilde{E}(M)=\{x\in E(M) \mid \forall f\in S, f(M)=0 \implies f(x)=0\}\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In general, there may be maps in &#039;&#039;S&#039;&#039; which are zero on &#039;&#039;M&#039;&#039; and yet are nonzero for some &#039;&#039;x&#039;&#039; not in &#039;&#039;M&#039;&#039;, and such an &#039;&#039;x&#039;&#039; would not be in the rational hull.&lt;br /&gt;
&lt;br /&gt;
=== Maximal right ring of quotients ===&lt;br /&gt;
{{main|Maximal ring of quotients}}&lt;br /&gt;
&lt;br /&gt;
The maximal right ring of quotients can be described in two ways in connection with dense right ideals of &#039;&#039;R&#039;&#039;.&lt;br /&gt;
* In one method, &#039;&#039;Ẽ&#039;&#039;(&#039;&#039;R&#039;&#039;) is shown to be module isomorphic to a certain endomorphism ring, and the ring structure is taken across this isomorphism to imbue &#039;&#039;Ẽ&#039;&#039;(&#039;&#039;R&#039;&#039;) with a ring structure, that of the maximal right ring of quotients. {{harv|Lam|1999|p=366}}&lt;br /&gt;
 &lt;br /&gt;
* In a second method, the maximal right ring of quotients is identified with a set of [[equivalence class]]es of homomorphisms from dense right ideals of &#039;&#039;R&#039;&#039; into &#039;&#039;R&#039;&#039;.  The equivalence relation says that two functions are equivalent if they agree on a dense right ideal of &#039;&#039;R&#039;&#039;. {{harv|Lam|1999|p=370}}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;!--- See http://en.wikipedia.org/wiki/Wikipedia:Footnotes on how to create references using &amp;lt;ref&amp;gt;&amp;lt;/ref&amp;gt; tags which will then appear here automatically --&amp;gt;&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
*{{citation&lt;br /&gt;
  |author1=Findlay, G. D.&lt;br /&gt;
  |author2=Lambek, J.&lt;br /&gt;
  |title=A generalized ring of quotients. I, II&lt;br /&gt;
  |journal=[[Canadian Mathematical Bulletin]]&lt;br /&gt;
  |volume=1&lt;br /&gt;
  |year=1958&lt;br /&gt;
  |pages=77–85, 155–167&lt;br /&gt;
  |issn=0008-4395&lt;br /&gt;
  |mr=0094370 (20 #888)}}&lt;br /&gt;
*{{citation&lt;br /&gt;
  |author=Johnson, R. E.&lt;br /&gt;
  |title=The extended centralizer of a ring over a module&lt;br /&gt;
  |journal=Proc. Amer. Math. Soc.&lt;br /&gt;
  |volume=2&lt;br /&gt;
  |year=1951&lt;br /&gt;
  |pages=891–895&lt;br /&gt;
  |issn=0002-9939&lt;br /&gt;
  |mr=0045695 (13,618c)}}&lt;br /&gt;
*{{Citation | last1=Lam | first1=Tsit-Yuen | title=Lectures on modules and rings | publisher=[[Springer-Verlag]] | location=Berlin, New York | series=Graduate Texts in Mathematics No. 189 | isbn=978-0-387-98428-5 | mr=1653294 | year=1999}}&lt;br /&gt;
*{{citation&lt;br /&gt;
  |author=Storrer, Hans H.&lt;br /&gt;
  |title=On Goldman&#039;s primary decomposition&lt;br /&gt;
  |journal=Lecutres on rings and modules (Tulane Univ. Ring and Operator Theory) &lt;br /&gt;
  |year=1970–1971 &lt;br /&gt;
  |volume= I&lt;br /&gt;
  |publisher=Springer&lt;br /&gt;
  |place=Berlin&lt;br /&gt;
  |year=1972&lt;br /&gt;
  |pages=617–661. Lecture Notes in Math., Vol. 246&lt;br /&gt;
  |mr=0360717 (50 #13164)}}&lt;br /&gt;
*{{citation&lt;br /&gt;
  |author=Utumi, Yuzo&lt;br /&gt;
  |title=On quotient rings&lt;br /&gt;
  |journal=Osaka Math. J.&lt;br /&gt;
  |volume=8&lt;br /&gt;
  |year=1956&lt;br /&gt;
  |pages=1–18&lt;br /&gt;
  |mr=0078966 (18,7c)}}&lt;br /&gt;
&amp;lt;!--- Categories ---&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Category:Abstract algebra]]&lt;br /&gt;
[[Category:Module theory]]&lt;br /&gt;
[[Category:Ring theory]]&lt;/div&gt;</summary>
		<author><name>131.111.20.56</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Cyclotomic_polynomial&amp;diff=2612</id>
		<title>Cyclotomic polynomial</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Cyclotomic_polynomial&amp;diff=2612"/>
		<updated>2014-01-19T15:03:09Z</updated>

		<summary type="html">&lt;p&gt;131.111.184.25: /* Easy cases for the computation */  statement is not true for n = 1&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{no footnotes|date=February 2013}}&lt;br /&gt;
An &#039;&#039;&#039;adaptive filter&#039;&#039;&#039; is a filter that self-adjusts its [[transfer function]] according to an optimization algorithm driven by an error signal.  Because of the complexity of the optimization algorithms, most adaptive filters are [[digital filter]]s. By way of contrast, a non-adaptive filter has a static transfer function. Adaptive filters are required for some applications because some parameters of the desired processing operation (for instance, the locations of reflective surfaces in a [[reverberant]] space) are not known in advance. The adaptive filter uses feedback in the form of an error signal to refine its transfer function to match the changing parameters.&lt;br /&gt;
&lt;br /&gt;
Generally speaking, the adaptive process involves the use of a [[Loss function|cost function]], which is a criterion for optimum performance of the filter, to feed an algorithm, which determines how to modify filter transfer function to minimize the cost on the next iteration.&lt;br /&gt;
&lt;br /&gt;
As the power of [[digital signal processor]]s has increased, adaptive filters have become much more common and are now routinely used in devices such as mobile phones and other communication devices, camcorders and digital cameras, and medical monitoring equipment.&lt;br /&gt;
&lt;br /&gt;
==Example application==&lt;br /&gt;
Suppose a [[hospital]] is recording a heart beat (an [[ECG]]), which is being corrupted by a 60 [[Hertz|Hz]] noise (the frequency coming from the [[power supply]] in many countries). However, due to slight variations in the power supply to the hospital, the noise signal may contain [[harmonics]] of the noise and the exact frequency of the noise may vary.&lt;br /&gt;
&lt;br /&gt;
One way to remove the noise is to filter the signal with a [[notch filter]] at 60 Hz. Such a static filter would need to remove all the frequencies in the vicinity of 60 Hz, which could excessively degrade the quality of the ECG since the heart beat would also likely have frequency components in the rejected range.&lt;br /&gt;
&lt;br /&gt;
To circumvent this potential loss of information, an adaptive filter could be used. The adaptive filter would take input both from the patient and from the power supply directly and would thus be able to track the actual frequency of the noise as it fluctuates. Such an adaptive technique generally allows for a filter with a smaller rejection range, which means, in our case, that the quality of the output signal is more accurate for medical diagnoses .&lt;br /&gt;
&lt;br /&gt;
==Block diagram==&lt;br /&gt;
The block diagram, shown in the following figure, serves as a foundation for particular adaptive filter realisations, such as [[Least mean squares filter|Least Mean Squares (LMS)]] and [[Recursive least squares filter|Recursive Least Squares (RLS)]]. The idea behind the block diagram is that a variable filter extracts an estimate of the desired signal.&lt;br /&gt;
:[[Image:AdaptiveFilter C.png|500px|Block diagram]]&lt;br /&gt;
To start the discussion of the block diagram we take the following assumptions:&lt;br /&gt;
*The input signal is the sum of a desired signal &amp;lt;math&amp;gt; d(n)&amp;lt;/math&amp;gt; and interfering noise &amp;lt;math&amp;gt; v(n)&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; x(n) = d(n)+v(n)&amp;lt;/math&amp;gt;&lt;br /&gt;
*The variable filter has a [[Finite impulse response|Finite Impulse Response (FIR)]] structure. For such structures the impulse response is equal to the filter coefficients. The coefficients for a filter of order &amp;lt;math&amp;gt; p&amp;lt;/math&amp;gt; are defined as&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbf{w}_{n}=\left[w_{n}(0),\,w_{n}(1),\, ...,\,w_{n}(p)\right]^{T}&amp;lt;/math&amp;gt;.&lt;br /&gt;
*The error signal or [[Loss function|cost function]] is the difference between the desired and the estimated signal&lt;br /&gt;
:&amp;lt;math&amp;gt; e(n) = d(n)-\hat{d}(n)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The variable filter estimates the desired signal by convolving the input signal with the impulse response. In vector notation this is expressed as&lt;br /&gt;
:&amp;lt;math&amp;gt; \hat{d}(n) = \mathbf{w}_{n}*\mathbf{x}(n)&amp;lt;/math&amp;gt;&lt;br /&gt;
where&lt;br /&gt;
:&amp;lt;math&amp;gt; \mathbf{x}(n)=\left[x(n),\,x(n-1),\,...,\,x(n-p)\right]^{T}&amp;lt;/math&amp;gt;&lt;br /&gt;
is an input signal vector. Moreover, the variable filter updates the filter coefficients at every time instant&lt;br /&gt;
:&amp;lt;math&amp;gt; \mathbf{w}_{n+1} = \mathbf{w}_{n}+\Delta\mathbf{w}_{n}&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\Delta\mathbf{w}_{n}&amp;lt;/math&amp;gt; is a correction factor for the filter coefficients. The adaptive algorithm generates this correction factor based on the input and error signals. LMS and RLS  define two different coefficient update algorithms.&lt;br /&gt;
&lt;br /&gt;
== Applications of adaptive filters ==&lt;br /&gt;
* [[Noise cancellation]]&lt;br /&gt;
* [[Linear prediction|Signal prediction]]&lt;br /&gt;
* [[Adaptive feedback cancellation]]&lt;br /&gt;
* [[Echo cancellation]]&lt;br /&gt;
&lt;br /&gt;
==Filter implementations==&lt;br /&gt;
*[[Least mean squares filter]]&lt;br /&gt;
*[[Recursive least squares filter]]&lt;br /&gt;
*[[Multidelay block frequency domain adaptive filter]]&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Kalman filter]]&lt;br /&gt;
*[[Wiener filter]]&lt;br /&gt;
*[[Linear prediction]]&lt;br /&gt;
*[[Filter (signal processing)]]&lt;br /&gt;
*[[Kernel adaptive filter]]&lt;br /&gt;
*[[Wiener-Hopf equation]]&lt;br /&gt;
*[[MMSE estimator]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*{{cite book |last=Hayes |first=Monson H. |authorlink= |title=Statistical Digital Signal Processing and Modeling |year=1996 |publisher=Wiley |location= |isbn=0-471-59431-8}}&lt;br /&gt;
*{{cite book |last=Haykin |first=Simon |authorlink= |title=Adaptive Filter Theory |year=2002 |publisher=Prentice Hall |location= |isbn=0-13-048434-2}}&lt;br /&gt;
*{{cite book |last1=Widrow |first1=Bernard |last2=Stearns |first2=Samuel D. |title=Adaptive Signal Processing |year=1985 |publisher=Prentice Hall |location=Englewood Cliffs, NJ |isbn=0-13-004029-0}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Adaptive Filter}}&lt;br /&gt;
[[Category:Digital signal processing]]&lt;br /&gt;
[[Category:Nonlinear filters]]&lt;/div&gt;</summary>
		<author><name>131.111.184.25</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Eigenfunction&amp;diff=3169</id>
		<title>Eigenfunction</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Eigenfunction&amp;diff=3169"/>
		<updated>2014-01-09T13:54:16Z</updated>

		<summary type="html">&lt;p&gt;131.111.184.10: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Quantification&#039;&#039;&#039; has several distinct senses. In [[mathematics]] and [[empirical science]], it is the act of [[counting]] and [[measuring]] that maps human sense [[observation]]s and [[experience]]s into [[element (mathematics)|member]]s of some [[Set (mathematics)|set]] of [[number]]s. Quantification in this sense is fundamental to the [[scientific method]]. &lt;br /&gt;
&lt;br /&gt;
In [[logic]], &#039;&#039;&#039;quantification&#039;&#039;&#039; is the binding of a variable ranging over a [[domain of discourse]]. The variable thereby becomes [[bound variable|bound]] by an [[variable binding operator|operator]] called a  &#039;&#039;&#039;quantifier&#039;&#039;&#039;. Academic discussion of quantification refers more often to this meaning of the term than the preceding one. &lt;br /&gt;
&lt;br /&gt;
In grammar, a &#039;&#039;&#039;quantifier&#039;&#039;&#039; is a type of [[Determiner (class)|determiner]], such as &#039;&#039;all&#039;&#039; or &#039;&#039;many&#039;&#039;, that indicates quantity. These items have been argued to correspond to logical quantifiers at the semantic level.&lt;br /&gt;
&lt;br /&gt;
==Natural language==&lt;br /&gt;
{{See also|Number names}}&lt;br /&gt;
All known human languages make use of quantification (Wiese 2004).  For example, in English:&lt;br /&gt;
* &#039;&#039;Every&#039;&#039; glass in my recent order was chipped.&lt;br /&gt;
* &#039;&#039;Some of&#039;&#039; the people standing across the river have white armbands.&lt;br /&gt;
* &#039;&#039;Most of&#039;&#039; the people I talked to didn&#039;t have a clue who  the candidates were.&lt;br /&gt;
* &#039;&#039;A lot of&#039;&#039; people are smart.&lt;br /&gt;
&lt;br /&gt;
The words in italics are quantifiers. &lt;br /&gt;
There exists no simple way of reformulating any one of these expressions as a conjunction or disjunction of sentences, each a simple predicate of an individual such as &#039;&#039;That wine glass was chipped&#039;&#039;.  These examples also suggest that the construction of quantified expressions in natural language can be syntactically very complicated.  Fortunately, for mathematical assertions, the quantification process is syntactically more straightforward.&lt;br /&gt;
&lt;br /&gt;
The study of quantification in natural languages is much more difficult than the corresponding problem for formal languages. This comes in part from the fact that the grammatical structure of natural language sentences may conceal the logical structure. Moreover, mathematical conventions strictly specify the range of validity for formal language quantifiers; for natural language, specifying the range of validity requires dealing with non-trivial semantic problems. For example the sentence ″&#039;&#039;Someone gets mugged in New York every 10 minutes&#039;&#039;″ does not identify whether it is the same person getting mugged every 10 minutes.&lt;br /&gt;
&lt;br /&gt;
[[Montague grammar]] gives a novel formal semantics of natural languages. Its proponents argue that it provides a much more natural formal rendering of natural language than the traditional treatments of [[Gottlob Frege|Frege]], [[Bertrand Russell|Russell]] and [[Willard Van Orman Quine|Quine]].&lt;br /&gt;
&lt;br /&gt;
==Logic==&lt;br /&gt;
{{see also|generalized quantifier|Lindström quantifier}}&lt;br /&gt;
&lt;br /&gt;
In [[language]] and [[logic]], quantification is a construct that specifies the quantity of specimens in the [[domain of discourse]] that apply to (or satisfy) an open formula. For example, in arithmetic, it allows the expression of the statement that every natural number has a successor. A language element which generates a quantification is called a quantifier. The resulting expression is a quantified expression; and the expression is said to be quantified over the predicate or function expression whose [[Free variables and bound variables|free variable]] is [[bound variable|bound]] by the quantifier. Quantification is used in both [[natural language]]s and [[formal language]]s. Examples of quantifiers in English are &#039;&#039;for all&#039;&#039;, &#039;&#039;for some&#039;&#039;, &#039;&#039;many&#039;&#039;, &#039;&#039;few&#039;&#039;, &#039;&#039;a lot&#039;&#039;, and &#039;&#039;no&#039;&#039;. In formal languages, quantification is a formula constructor that produces new formulas from old ones.  The [[semantics]] of the language specifies how the constructor is interpreted as an extent of validity.&lt;br /&gt;
&lt;br /&gt;
The two fundamental kinds of quantification in [[predicate (logic)|predicate logic]] are [[universal quantification]] and [[existential quantification]]. The traditional symbol for the universal quantifier &amp;quot;all&amp;quot; is &amp;quot;∀&amp;quot;, an inverted letter &amp;quot;[[A]]&amp;quot;, and for the [[existential quantification|existential quantifier]] &amp;quot;exists&amp;quot; is  &amp;quot;∃&amp;quot;, a rotated letter &amp;quot;[[E]]&amp;quot;. These quantifiers have been generalized beginning with the work of [[Andrzej Mostowski|Mostowski]] and [[Per Lindström|Lindström]].&lt;br /&gt;
&lt;br /&gt;
===Mathematics===&lt;br /&gt;
Consider the following statement:&lt;br /&gt;
: 1·2 = 1 + 1, and 2·2 = 2 + 2, and 3 · 2 = 3 + 3, ...., and &#039;&#039;n&#039;&#039; · 2 = &#039;&#039;n&#039;&#039; + &#039;&#039;n&#039;&#039;, etc.&lt;br /&gt;
This has the appearance of an &#039;&#039;infinite [[logical conjunction|conjunction]]&#039;&#039; of propositions.  From the point of view of [[formal language]]s this is immediately a problem, since [[syntax]] rules are expected to generate [[finite set|finite]] objects. The example above is fortunate in that there is a [[Algorithm|procedure]] to generate all the conjuncts.  However, if an assertion were to be made about every [[irrational number]], there would be no way to enumerate all the conjuncts, since irrationals cannot be enumerated. A succinct formulation which avoids these problems uses &#039;&#039;universal quantification&#039;&#039;:&lt;br /&gt;
: For any [[natural number]] &#039;&#039;n&#039;&#039;, &#039;&#039;n&#039;&#039;·2 = &#039;&#039;n&#039;&#039; + &#039;&#039;n&#039;&#039;.&lt;br /&gt;
A similar analysis applies to the [[disjunction (logic)|disjunction]],&lt;br /&gt;
: 1 is equal to 5 + 5, or 2 is equal to 5 + 5, or 3 is equal to 5 + 5, ... , or n is equal to 5 + 5, etc.&lt;br /&gt;
which can be rephrased using &#039;&#039;existential quantification&#039;&#039;:&lt;br /&gt;
: For some [[natural number]] &#039;&#039;n&#039;&#039;, &#039;&#039;n&#039;&#039; is equal to 5 + 5.&lt;br /&gt;
&lt;br /&gt;
It is possible to devise [[abstract algebra]]s whose [[model theory|models]] include [[formal language]]s with quantification, but progress has been slow and interest in such algebra has been limited. Three approaches have been devised to date:&lt;br /&gt;
* [[Relation algebra]], invented by [[De Morgan]], and developed by [[Charles Sanders Peirce]], [[Ernst Schröder]], [[Tarski]], and Tarski&#039;s students. Relation algebra cannot represent any formula with quantifiers nested more than three deep. Surprisingly, the [[model theory|models]] of relation algebra include the [[axiomatic set theory]] [[ZFC]] and [[Peano arithmetic]];&lt;br /&gt;
* [[Cylindric algebra]], devised by [[Tarski]], [[Henkin]], and others;&lt;br /&gt;
* The [[polyadic algebra]] of [[Paul Halmos]].&lt;br /&gt;
&lt;br /&gt;
===Notation===&lt;br /&gt;
There are two quantifiers, the universal quantifier and the existential quantifier. The traditional symbol for the universal quantifier is &amp;quot;∀&amp;quot;, an inverted letter &amp;quot;[[A]]&amp;quot;, which stands for  &amp;quot;for all&amp;quot; or &amp;quot;all&amp;quot;.  The corresponding symbol for the existential quantifier is &amp;quot;∃&amp;quot;, a rotated letter &amp;quot;[[E]]&amp;quot;, which stands for &amp;quot;there exists&amp;quot; or &amp;quot;exists&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
An example of quantifying an English statement would be as follows. Given the statement, &amp;quot;All of Peters friends either like to dance or like to go to the beach&amp;quot;, we can identify key aspects and rewrite using symbols including quantifiers. So, let x be any one particular friend of Peter, X the set of all Peter&#039;s friends, P(x) be the [[predicate]] (mathematical logic) &amp;quot;x likes to dance&amp;quot;, and lastly Q(x) the predicate &amp;quot;x likes to go to the beach&amp;quot;. Then we have, : &amp;lt;math&amp;gt; \forall{x}{\in}X, P(x) \or Q(x) &amp;lt;/math&amp;gt;. Which is read, &amp;quot;for all x that&#039;s a member of X, P of x or Q of x.&amp;quot;&lt;br /&gt;
&lt;br /&gt;
Some other quantified expressions are constructed as follows, &lt;br /&gt;
: &amp;lt;math&amp;gt; \exists{x}\, P  \qquad \forall{x}\, P &amp;lt;/math&amp;gt;&lt;br /&gt;
for a formula &#039;&#039;P&#039;&#039;. Variant notations include, for set &#039;&#039;X&#039;&#039; and set members &#039;&#039;x&#039;&#039;:&lt;br /&gt;
: &amp;lt;math&amp;gt; (\exists{x}) P \qquad (\exists x \ . \ P) \qquad \exists x \ \cdot \ P \qquad (\exists x : P) \qquad \exists{x}(P) \qquad \exists_{x}\, P \qquad \exists{x}{,}\, P \qquad \exists{x}{\in}X \, P \qquad \exists\, x{:}X \, P&amp;lt;/math&amp;gt;&lt;br /&gt;
All of these variations also apply to universal quantification.&lt;br /&gt;
Other variations for the universal quantifier are&lt;br /&gt;
: &amp;lt;math&amp;gt;(x) \, P \qquad \bigwedge_{x} P&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Some versions of the notation explicitly mention the range of quantification.  The range of quantification must always be specified; for a given mathematical theory, this can be done in several ways:&lt;br /&gt;
* Assume a fixed domain of discourse for every quantification, as is done in [[Zermelo–Fraenkel set theory]],&lt;br /&gt;
* Fix several domains of discourse in advance and require that each variable have a declared domain, which is the &#039;&#039;type&#039;&#039; of that variable. This is analogous to the situation in [[Type system|statically typed]] [[computer programming]] languages, where variables have declared types.&lt;br /&gt;
* Mention explicitly the range of quantification, perhaps using a symbol for the set of all objects in that domain or the [[type (logic)|type]] of the objects in that domain.&lt;br /&gt;
&lt;br /&gt;
One can use any variable as a quantified variable in place of any other, under certain restrictions in which &#039;&#039;variable capture&#039;&#039; does not occur.  Even if the notation uses typed variables, variables of that type may be used. &lt;br /&gt;
&lt;br /&gt;
Informally or in natural language, the &amp;quot;∀&#039;&#039;x&#039;&#039;&amp;quot; or &amp;quot;∃&#039;&#039;x&#039;&#039;&amp;quot; might appear after or in the middle of &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;). Formally, however, the phrase that introduces the dummy variable is placed in front.&lt;br /&gt;
&lt;br /&gt;
Mathematical formulas mix symbolic expressions for quantifiers, with natural language quantifiers such as&lt;br /&gt;
: For any natural number &#039;&#039;x&#039;&#039;, ....&lt;br /&gt;
: There exists an &#039;&#039;x&#039;&#039; such that ....&lt;br /&gt;
: For at least one &#039;&#039;x&#039;&#039;.&lt;br /&gt;
Keywords for [[uniqueness quantification]] include:&lt;br /&gt;
: For exactly one natural number &#039;&#039;x&#039;&#039;, ....&lt;br /&gt;
: There is one and only one &#039;&#039;x&#039;&#039; such that ....&lt;br /&gt;
Further, &#039;&#039;x&#039;&#039; may be replaced by a [[pronoun]]. For example, &lt;br /&gt;
:For any natural number, its product with 2 equals to its sum with itself&lt;br /&gt;
:Some natural number is prime.&lt;br /&gt;
&lt;br /&gt;
===Equivalent expressions===&lt;br /&gt;
If &#039;&#039;X&#039;&#039; is a domain of &#039;&#039;x&#039;&#039; and &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;) is a predicate dependent on &#039;&#039;x&#039;&#039;, then the universal proposition is expressed in [[Boolean algebra]] terms as&amp;lt;br /&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\forall x\in X, P(x) \equiv \{x\in X\} \rightarrow P(x) \equiv \{x\notin X\} \or P(x),&amp;lt;/math&amp;gt;&lt;br /&gt;
which equivalently reads &amp;quot;if &#039;&#039;x&#039;&#039; is in &#039;&#039;X&#039;&#039;, then &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;) is true.&amp;quot; If &#039;&#039;x&#039;&#039; is not in &#039;&#039;X&#039;&#039;, then &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;) is indeterminate. Note that the truth of the expression requires only that &#039;&#039;x&#039;&#039; be in &#039;&#039;X&#039;&#039;, so it can be &#039;&#039;any x&#039;&#039; in &#039;&#039;X&#039;&#039;, independent of &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;), whereas the &#039;&#039;falsity&#039;&#039; of the expression, or the truth of&lt;br /&gt;
:&amp;lt;math&amp;gt;\{x\in X\} \and \neg P(x),&amp;lt;/math&amp;gt;&lt;br /&gt;
additionally requires that &#039;&#039;x&#039;&#039; be such that &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;) evaluates to false; this is the reason behind calling &#039;&#039;x&#039;&#039; a &amp;quot;bound variable.&amp;quot; This last expression can thus be read as &amp;quot;for some &#039;&#039;x&#039;&#039; in &#039;&#039;X&#039;&#039;, &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;) is false,&amp;quot; or &amp;quot;there exists an &#039;&#039;x&#039;&#039; in &#039;&#039;X&#039;&#039; such that &#039;&#039;P&#039;&#039;(&#039;&#039;x&#039;&#039;) is false.&amp;quot; So, we now have the equivalent Boolean expression for the existential proposition:&amp;lt;br /&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\exists x\in X : P(x) \equiv \{x\in X\} \and P(x).&amp;lt;/math&amp;gt;&lt;br /&gt;
Thus, together with negation, only one of either the universal or existential quantifier is needed to perform both tasks:&lt;br /&gt;
:&amp;lt;math&amp;gt;\neg (\forall x\in X, P(x)) \equiv \exists x\in X : \neg P(x), &amp;lt;/math&amp;gt;&lt;br /&gt;
which shows that to disprove a &amp;quot;for all &#039;&#039;x&#039;&#039;&amp;quot; proposition, one needs no more than to find an &#039;&#039;x&#039;&#039; for which the predicate is false. Similarly,&amp;lt;br /&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\neg (\exists x\in X : P(x)) \equiv \forall x\in X, \neg P(x), &amp;lt;/math&amp;gt;&lt;br /&gt;
to disprove a &amp;quot;there exists an &#039;&#039;x&#039;&#039;&amp;quot; proposition, one needs to show that the predicate is false for all &#039;&#039;x&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
===Nesting===&lt;br /&gt;
Consider the following statement:&lt;br /&gt;
:For any natural number &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt;, there is a natural number &amp;lt;math&amp;gt;s&amp;lt;/math&amp;gt; such that &amp;lt;math&amp;gt;s = n^2 &amp;lt;/math&amp;gt;.&lt;br /&gt;
This is clearly true; it just asserts that every natural number has a square. The meaning of the assertion in which the quantifiers are turned around is different:&lt;br /&gt;
: There is a natural number &amp;lt;math&amp;gt;s&amp;lt;/math&amp;gt; such that for any natural number &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;s = n^2&amp;lt;/math&amp;gt;.&lt;br /&gt;
This is clearly false; it asserts that there is a single natural number &#039;&#039;s&#039;&#039; that is at once the square of &#039;&#039;every&#039;&#039; natural number. This is because the syntax directs that any newly introduced variable cannot be a function of subsequently introduced variables.&lt;br /&gt;
&lt;br /&gt;
This illustrates that the order of quantifiers is critical to meaning.&lt;br /&gt;
&lt;br /&gt;
A less trivial example is the important concept of [[uniform continuity]]  from [[mathematical analysis|analysis]], which differs from the more familiar concept of [[continuous function|pointwise continuity]] only by an exchange in the positions of two quantifiers.&lt;br /&gt;
To illustrate this, let &#039;&#039;f&#039;&#039; be a real-valued function on &#039;&#039;&#039;R&#039;&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
* A: Pointwise continuity of &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; on &#039;&#039;&#039;R&#039;&#039;&#039;:&lt;br /&gt;
::&amp;lt;math&amp;gt; \underbrace{\forall x \in \mathbb{R} \, \, \forall \epsilon &amp;gt;0} \, \exists \delta &amp;gt; 0 \, \forall h \in \mathbb{R} \, \left( \, |h| &amp;lt; \delta \, \to \,  |f(x) - f(x+h)| &amp;lt; \epsilon \, \right) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
interchanging the universal quantifiers over the braces, this is the same as &lt;br /&gt;
* A&#039;: Pointwise continuity of &#039;&#039;f&#039;&#039; on &#039;&#039;&#039;R&#039;&#039;&#039;:&lt;br /&gt;
::&amp;lt;math&amp;gt; \forall \epsilon &amp;gt;0 \, \underbrace{\forall x \in \mathbb{R} \, \, \exists \delta &amp;gt; 0} \, \forall h \in \mathbb{R} \, \left( \, |h| &amp;lt; \delta  \, \to \, |f(x) - f(x+h)| &amp;lt; \epsilon \, \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus, it is implied that the particular value chosen for &#039;&#039;δ&#039;&#039; can only be a function of &#039;&#039;ε&#039;&#039; and &#039;&#039;x&#039;&#039;, the variables that precede it; whereas in&lt;br /&gt;
* B: Uniform continuity of &#039;&#039;f&#039;&#039; on &#039;&#039;&#039;R&#039;&#039;&#039;:&lt;br /&gt;
::&amp;lt;math&amp;gt; \forall \epsilon &amp;gt;0 \, \underbrace{\exists \delta &amp;gt; 0 \, \, \forall x \in \mathbb{R}} \,  \forall h \in \mathbb{R} \, \left( \, |h| &amp;lt; \delta \, \to \, |f(x) - f(x+h)| &amp;lt; \epsilon \, \right) &amp;lt;/math&amp;gt;&lt;br /&gt;
by interchanging the existential and universal quantifiers over the braces in A&#039;, &#039;&#039;δ&#039;&#039; is asserted to be independent of &#039;&#039;x&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
Ambiguity is avoided with the quantifiers in front:&lt;br /&gt;
*&amp;lt;math&amp;gt; \exists&amp;lt;/math&amp;gt; A:&amp;lt;math&amp;gt; \forall&amp;lt;/math&amp;gt; B: C – unambiguous&lt;br /&gt;
*there is an A such that &amp;lt;math&amp;gt;\forall&amp;lt;/math&amp;gt; B: C – unambiguous&lt;br /&gt;
*there is an A such that for all B, C – unambiguous, provided that the separation between B and C is clear&lt;br /&gt;
*there is an A such that C for all B – it is often clear that what is meant is&lt;br /&gt;
:: there is an A such that (C for all B)&lt;br /&gt;
:but it could be interpreted as&lt;br /&gt;
:: (there is an A such that C) for all B&lt;br /&gt;
*there is an A such that C &amp;lt;math&amp;gt;\forall&amp;lt;/math&amp;gt; B &amp;amp;mdash; suggests more strongly that the first is meant; this may be reinforced by the layout, for example by putting &amp;quot;C &amp;lt;math&amp;gt;\forall&amp;lt;/math&amp;gt; B&amp;quot; on a new line.&lt;br /&gt;
&lt;br /&gt;
The maximum depth of nesting of quantifiers inside a formula is called its [[Quantifier rank]].&lt;br /&gt;
&lt;br /&gt;
===Range of quantification===&lt;br /&gt;
Every quantification involves one specific variable and a &#039;&#039;domain of discourse&#039;&#039; or &#039;&#039;range of quantification&#039;&#039; of that variable.  The range of quantification specifies the set of values that the variable takes.  In the examples above, the range of quantification is the set of natural numbers.  Specification of the range of quantification allows us to express the difference between, asserting that a predicate holds for some natural number or for some [[real number]]. Expository conventions often reserve some variable names such as &amp;quot;&#039;&#039;n&#039;&#039;&amp;quot; for natural numbers and &amp;quot;&#039;&#039;x&#039;&#039;&amp;quot; for real numbers, although relying exclusively on naming conventions cannot work in general since ranges of variables can change in the course of a mathematical argument. &lt;br /&gt;
&lt;br /&gt;
A more natural way to restrict the domain of discourse uses &#039;&#039;guarded quantification&#039;&#039;.  For example, the guarded quantification &lt;br /&gt;
:For some natural number &#039;&#039;n&#039;&#039;, &#039;&#039;n&#039;&#039; is even and &#039;&#039;n&#039;&#039; is prime&lt;br /&gt;
means&lt;br /&gt;
:For some [[even number]] &#039;&#039;n&#039;&#039;, &#039;&#039;n&#039;&#039; is prime.&lt;br /&gt;
&lt;br /&gt;
In some mathematical theories a single domain of&lt;br /&gt;
discourse fixed in advance is assumed.  For example, in [[Zermelo–Fraenkel set theory]], variables range over all sets.  In this case, guarded quantifiers can be used to mimic a smaller range of quantification.  Thus in the example&lt;br /&gt;
above to express&lt;br /&gt;
:For any natural number &#039;&#039;n&#039;&#039;, &#039;&#039;n&#039;&#039;·2 = &#039;&#039;n&#039;&#039; + &#039;&#039;n&#039;&#039;&lt;br /&gt;
in Zermelo–Fraenkel set theory, it can be said&lt;br /&gt;
:For any &#039;&#039;n&#039;&#039;, if &#039;&#039;n&#039;&#039; belongs to &#039;&#039;&#039;N&#039;&#039;&#039;, then &#039;&#039;n&#039;&#039;·2 = &#039;&#039;n&#039;&#039; + &#039;&#039;n&#039;&#039;,&lt;br /&gt;
where &#039;&#039;&#039;N&#039;&#039;&#039; is the set of all natural numbers.&lt;br /&gt;
&lt;br /&gt;
===Formal semantics===&lt;br /&gt;
Mathematical Semantics is the application of [[mathematics]] to study the meaning of expressions in a formal language. It has three elements: A mathematical specification of a class of objects via [[syntax]], a mathematical specification of various semantic domains and the relation between the two, which is usually expressed as a function from syntactic objects to semantic ones.  This article only addresses the issue of how quantifier elements are interpreted.&lt;br /&gt;
&lt;br /&gt;
Given a [[model theory|model theoretical]] logical framework, the syntax of a formula can be given by a syntax tree. Quantifiers have scope and a variable &#039;&#039;x&#039;&#039; is [[free variable|free]] if it is not within the scope of a quantification for that variable. Thus in&lt;br /&gt;
:&amp;lt;math&amp;gt; \forall x (\exists y  B(x,y)) \vee C(y,x) &amp;lt;/math&amp;gt;&lt;br /&gt;
the occurrence of both &#039;&#039;x&#039;&#039; and &#039;&#039;y&#039;&#039; in &#039;&#039;C&#039;&#039;(&#039;&#039;y&#039;&#039;,&#039;&#039;x&#039;&#039;) is free.&lt;br /&gt;
&lt;br /&gt;
[[File:IMG Tree.gif|thumb|230px|right|Syntactic tree illustrating scope and variable capture]]&lt;br /&gt;
An interpretation for first-order predicate calculus assumes as given&lt;br /&gt;
a domain of individuals &#039;&#039;X&#039;&#039;.  A formula &#039;&#039;A&#039;&#039; whose free variables&lt;br /&gt;
are &#039;&#039;x&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ..., &#039;&#039;x&#039;&#039;&amp;lt;sub&amp;gt;n&amp;lt;/sub&amp;gt; is interpreted as a&lt;br /&gt;
[[Boolean function|boolean]]-valued function &#039;&#039;F&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ...,&lt;br /&gt;
&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt;) of &#039;&#039;n&#039;&#039; arguments, where each argument ranges&lt;br /&gt;
over the domain &#039;&#039;X&#039;&#039;.  Boolean-valued means that the function assumes one of the values &#039;&#039;&#039;T&#039;&#039;&#039; (interpreted as truth) or &#039;&#039;&#039;F&#039;&#039;&#039; (interpreted as falsehood). The interpretation of the formula&lt;br /&gt;
:&amp;lt;math&amp;gt; \forall x_n A(x_1, \ldots , x_n) &amp;lt;/math&amp;gt;&lt;br /&gt;
is the function &#039;&#039;G&#039;&#039; of &#039;&#039;n&#039;&#039;-1 arguments such that &#039;&#039;G&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ...,&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt;) = &#039;&#039;&#039;T&#039;&#039;&#039; if and only if &#039;&#039;F&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ..., &#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt;, &#039;&#039;w&#039;&#039;) = &#039;&#039;&#039;T&#039;&#039;&#039; for every &#039;&#039;w&#039;&#039; in &#039;&#039;X&#039;&#039;. If  &#039;&#039;F&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ..., &#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt;, &#039;&#039;w&#039;&#039;) = &#039;&#039;&#039;F&#039;&#039;&#039; for at least one value of &#039;&#039;w&#039;&#039;, then &#039;&#039;G&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ...,&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt;) = &#039;&#039;&#039;F&#039;&#039;&#039;.  Similarly the interpretation of the formula&lt;br /&gt;
:&amp;lt;math&amp;gt; \exists x_n A(x_1, \ldots , x_n) &amp;lt;/math&amp;gt;&lt;br /&gt;
is the function &#039;&#039;H&#039;&#039; of &#039;&#039;n&#039;&#039;-1 arguments such that &#039;&#039;H&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ...,&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt;) = &#039;&#039;&#039;T&#039;&#039;&#039; if and only if &#039;&#039;F&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ...,&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt;, &#039;&#039;w&#039;&#039;) = &#039;&#039;&#039;T&#039;&#039;&#039; for at least one &#039;&#039;w&#039;&#039; and  &#039;&#039;H&#039;&#039;(&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;, ..., &#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt;) = &#039;&#039;&#039;F&#039;&#039;&#039; otherwise.&lt;br /&gt;
&lt;br /&gt;
The semantics for [[uniqueness quantification]] requires  first-order predicate calculus with equality. This means there is given a distinguished two-placed predicate &amp;quot;=&amp;quot;; the semantics is also modified accordingly so that &amp;quot;=&amp;quot; is always interpreted as the two-place equality relation on &#039;&#039;X&#039;&#039;. The interpretation of  &lt;br /&gt;
:&amp;lt;math&amp;gt; \exists !   x_n A(x_1, \ldots , x_n) &amp;lt;/math&amp;gt;&lt;br /&gt;
then is the function of &#039;&#039;n&#039;&#039;-1 arguments, which is the logical &#039;&#039;and&#039;&#039; of the interpretations of &lt;br /&gt;
:&amp;lt;math&amp;gt; \exists  x_n A(x_1, \ldots , x_n) &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; \forall y,z \left\{  A(x_1, \ldots ,x_{n-1}, y) \wedge  A(x_1, \ldots ,x_{n-1}, z) \implies y = z \right\}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Paucal, multal and other degree quantifiers===&lt;br /&gt;
{{See also|Fubini&#039;s theorem|measurable}}&lt;br /&gt;
&lt;br /&gt;
None of the quantifiers previously discussed apply to a quantification such as &lt;br /&gt;
&lt;br /&gt;
:There are many integers &#039;&#039;n&#039;&#039; &amp;lt; 100, such that &#039;&#039;n&#039;&#039; is divisible by 2 or 3 or 5.&lt;br /&gt;
&lt;br /&gt;
One possible interpretation mechanism can be obtained as follows: Suppose that in addition to a semantic domain &#039;&#039;X&#039;&#039;, we have given a [[probability measure]] P defined on &#039;&#039;X&#039;&#039; and cutoff numbers 0 &amp;lt; &#039;&#039;a&#039;&#039; ≤ &#039;&#039;b&#039;&#039; ≤  1.  If &#039;&#039;A&#039;&#039; is a formula with free variables &#039;&#039;x&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;,...,&#039;&#039;x&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt; whose interpretation is&lt;br /&gt;
the function &#039;&#039;F&#039;&#039; of variables &#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;,...,&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt;&lt;br /&gt;
then the interpretation of &lt;br /&gt;
:&amp;lt;math&amp;gt; \exists^{\mathrm{many}} x_n A(x_1, \ldots, x_{n-1}, x_n) &amp;lt;/math&amp;gt;&lt;br /&gt;
is the function of &#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;,...,&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt; which is &#039;&#039;&#039;T&#039;&#039;&#039; if and only if&lt;br /&gt;
:&amp;lt;math&amp;gt; \operatorname{P} \{w: F(v_1, \ldots, v_{n-1}, w) = \mathbf{T} \} \geq b &amp;lt;/math&amp;gt;&lt;br /&gt;
and &#039;&#039;&#039;F&#039;&#039;&#039; otherwise.  Similarly, the interpretation of &lt;br /&gt;
:&amp;lt;math&amp;gt; \exists^{\mathrm{few}}  x_n  A(x_1, \ldots, x_{n-1}, x_n) &amp;lt;/math&amp;gt;&lt;br /&gt;
is the function of &#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;,...,&#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;-1&amp;lt;/sub&amp;gt; which is &#039;&#039;&#039;F&#039;&#039;&#039; if and only if&lt;br /&gt;
:&amp;lt;math&amp;gt; 0&amp;lt; \operatorname{P} \{w: F(v_1, \ldots, v_{n-1}, w) = \mathbf{T}\} \leq a &amp;lt;/math&amp;gt;&lt;br /&gt;
and &#039;&#039;&#039;T&#039;&#039;&#039; otherwise.&lt;br /&gt;
&lt;br /&gt;
===Other quantifiers===&lt;br /&gt;
A few other quantifiers have been proposed over time. In particular, the solution quantifier,&amp;lt;ref&amp;gt;[[E. C. R. Hehner|Hehner, Eric C. R.]], 2004, [http://www.cs.utoronto.ca/~hehner/aPToP &#039;&#039;Practical Theory of Programming&#039;&#039;], 2nd edition, p. 28&amp;lt;/ref&amp;gt; noted § ([[section sign]]) and read &amp;quot;those&amp;quot;. For example:&lt;br /&gt;
:&amp;lt;math&amp;gt; \left [ \S n \in \mathbb{N} \quad n^2 \leq 4 \right ] = \left\{0, 1, 2\right\}&amp;lt;/math&amp;gt;&lt;br /&gt;
is read &amp;quot;those &#039;&#039;n&#039;&#039; in &#039;&#039;&#039;N&#039;&#039;&#039; such that &#039;&#039;n&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; ≤ 4 are in {0,1,2}.&amp;quot; The same construct is expressible in [[set-builder notation]]:&lt;br /&gt;
:&amp;lt;math&amp;gt;\{n \in \mathbf N: n^2 \le 4\} =  \left\{0, 1, 2\right\} \,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===History===&lt;br /&gt;
[[Term logic]] treats quantification in a manner that is closer to natural language, and also less suited to formal analysis. [[Aristotelian logic]] treated &#039;&#039;All&#039;&#039;, &#039;&#039;Some&#039;&#039;  and &#039;&#039;No&#039;&#039; in the 1st century BC, in an account also touching on the alethic modalities.&lt;br /&gt;
&lt;br /&gt;
[[Gottlob Frege]], in his 1879 &#039;&#039;[[Begriffsschrift]]&#039;&#039;, was the first to employ a quantifier to bind a variable ranging over a [[domain of discourse]] and appearing in [[Predicate (mathematical logic)|predicate]]s. He would universally quantify a variable (or relation) by writing the variable over a dimple in an otherwise straight line appearing in his diagrammatic formulas. Frege did not devise an explicit notation for existential quantification, instead employing his equivalent of ~∀&#039;&#039;x&#039;&#039;~, or [[contraposition]]. Frege&#039;s treatment of quantification went largely unremarked until [[Bertrand Russell]]&#039;s 1903 &#039;&#039;Principles of Mathematics&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
In work that culminated in Peirce (1885), [[Charles Sanders Peirce]] and his student [[Oscar Howard Mitchell]] independently invented universal and existential quantifiers, and [[bound variable]]s. Peirce and Mitchell wrote Π&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; and Σ&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; where we now write ∀&#039;&#039;x&#039;&#039; and ∃&#039;&#039;x&#039;&#039;. Peirce&#039;s notation can be found in the writings of [[Ernst Schröder]], [[Leopold Loewenheim]], [[Thoralf Skolem]], and Polish logicians into the 1950s. Most notably, it is the notation of [[Kurt Gödel]]&#039;s landmark 1930 paper on the [[Gödel&#039;s completeness theorem|completeness]] of [[first-order logic]], and 1931 paper on the [[Gödel&#039;s incompleteness theorem|incompleteness]] of [[Peano arithmetic]].&lt;br /&gt;
&lt;br /&gt;
Peirce&#039;s approach to quantification also influenced [[William Ernest Johnson]] and [[Giuseppe Peano]], who invented yet another notation, namely (&#039;&#039;x&#039;&#039;) for the universal quantification of &#039;&#039;x&#039;&#039; and (in 1897) ∃&#039;&#039;x&#039;&#039; for the existential quantification of &#039;&#039;x&#039;&#039;. Hence for decades, the canonical notation in philosophy and mathematical logic was (&#039;&#039;x&#039;&#039;)&#039;&#039;P&#039;&#039; to express &amp;quot;all individuals in the domain of discourse have the property &#039;&#039;P&#039;&#039;,&amp;quot; and &amp;quot;(∃&#039;&#039;x&#039;&#039;)&#039;&#039;P&#039;&#039;&amp;quot; for &amp;quot;there exists at least one individual in the domain of discourse having the property &#039;&#039;P&#039;&#039;.&amp;quot; Peano, who was much better known than Peirce, in effect diffused the latter&#039;s thinking throughout Europe. Peano&#039;s notation was adopted by the &#039;&#039;[[Principia Mathematica]]&#039;&#039; of [[Alfred North Whitehead|Whitehead]] and [[Bertrand Russell|Russell]], [[Willard Van Orman Quine|Quine]], and [[Alonzo Church]]. In 1935, [[Gentzen]] introduced the ∀ symbol, by analogy with Peano&#039;s ∃ symbol. ∀ did not become canonical until the 1960s.&lt;br /&gt;
&lt;br /&gt;
Around 1895, Peirce began developing his [[existential graph]]s, whose variables can be seen as tacitly quantified. Whether the shallowest instance of a variable is even or odd determines whether that variable&#039;s quantification is universal or existential. (Shallowness is the contrary of depth, which is determined by the nesting of negations.) Peirce&#039;s graphical logic has attracted some attention in recent years by those researching [[heterogeneous reasoning]] and [[logical graph|diagrammatic inference]].&lt;br /&gt;
&lt;br /&gt;
==Natural science==&lt;br /&gt;
Some measure of the undisputed general importance of quantification in the [[natural science]]s can be gleaned from the following comments: &amp;quot;these are mere facts, but they are quantitative facts and the basis of science.&amp;quot;&amp;lt;ref&amp;gt;[[James McKeen Cattell|Cattell, James McKeen]]; and [[Livingston Farrand|Farrand, Livingston]] (1896) &amp;quot;Physical and mental measurements of the students of Columbia University&amp;quot;, &#039;&#039;The Psychological Review&#039;&#039;, Vol.&amp;amp;nbsp;3, No.&amp;amp;nbsp;6 (1896), pp.&amp;amp;nbsp;618-648; p.&amp;amp;nbsp;648 quoted in &#039;&#039;[http://www.indiana.edu/~intell/jcattell.shtml James McKeen Cattell (1860-1944) Psychologist, Publisher, and Editor.]&#039;&#039;&amp;lt;/ref&amp;gt; It seems to be held as universally true that &amp;quot;the foundation of quantification is measurement.&amp;quot;&amp;lt;ref&amp;gt;[[Samuel Stanley Wilks|Wilks, Samuel Stanley]] (1961) &amp;quot;Some Aspects of Quantification in Science&amp;quot;, &#039;&#039;Isis&#039;&#039;, Vol.&amp;amp;nbsp;52, No.&amp;amp;nbsp;2 (1961), pp.&amp;amp;nbsp;135-142; p.&amp;amp;nbsp;135&amp;lt;/ref&amp;gt; There is little doubt that &amp;quot;quantification provided a basis for the objectivity of science.&amp;quot;&amp;lt;ref&amp;gt;Hong, Sungook (2004) &amp;quot;[http://www.sciencemag.org/cgi/content/full/305/5690/1569 History of Science: Building Circuits of Trust]&amp;quot;, &#039;&#039;Science&#039;&#039;, Vol.&amp;amp;nbsp;305, No.&amp;amp;nbsp;5690 (10 September 2004), pp.&amp;amp;nbsp;1569-1570&amp;lt;/ref&amp;gt; [The context of these quotes is slightly misleading - most scientists use quantification as related to quantities, which is categorically different than quantifier as used in this article.  Most would probably article that the word is Qualifier.] In ancient times, &amp;quot;musicians and artists...rejected quantification, but merchants, by definition, quantified their affairs, in order to survive, made them visible on parchment and paper.&amp;quot;&amp;lt;ref&amp;gt;[[Alfred W. Crosby|Crosby, Alfred W.]] (1996) &#039;&#039;The Measure of Reality: Quantification and Western Society&#039;&#039;, Cambridge University Press, 1996, p.&amp;amp;nbsp;201&amp;lt;/ref&amp;gt; Any reasonable &amp;quot;comparison between Aristotle and Galileo shows clearly that there can be no unique lawfulness discovered without detailed quantification.&amp;quot;&amp;lt;ref&amp;gt;Langs, Robert J. (1987) &amp;quot;[http://www.pep-web.org/document.php?id=cps.023.0555a Psychoanalysis as an Aristotelian Science—Pathways to Copernicus and a Modern-Day Approach]&amp;quot;, &#039;&#039;Contemporary Psychoanalysis&#039;&#039;, Vol.&amp;amp;nbsp;23 &amp;lt;!-- one vol. per year --&amp;gt;(1987), pp.&amp;amp;nbsp;555-576&amp;lt;/ref&amp;gt; Even today, &amp;quot;universities use imperfect instruments called &#039;[[exams]]&#039; to indirectly quantify something they call knowledge.&amp;quot;&amp;lt;ref&amp;gt;[[Aaron Lynch|Lynch, Aaron]] (1999) &amp;quot;[http://cfpm.org/jom-emit/1999/vol3/lynch_a.html Misleading Mix of Religion and Science,]&amp;quot; &#039;&#039;Journal of Memetics: Evolutionary Models of Information Transmission&#039;&#039;, Vol.&amp;amp;nbsp;3, No.&amp;amp;nbsp;1&amp;lt;!-- because there are only two issues, and there is Gatherer, Derek G. (1999) &amp;quot;Reply to Commentaries&amp;quot;, &#039;&#039;Journal of Memetics: Evolutionary Models of Information Transmission, Vol.&amp;amp;nbsp;3 [No.&amp;amp;nbsp;2] (1999) http://jom-emit.cfpm.org/1999/vol3/gatherer_reply.html --&amp;gt; (1999)&amp;lt;/ref&amp;gt; This meaning of quantification comes under the heading of [[Pragmatism|pragmatics]].&lt;br /&gt;
&lt;br /&gt;
In some instances in the natural sciences a seemingly intangible concept may be quantified by creating a scale—for example, a [[pain scale]] in medical research, or a discomfort scale at the intersection of [[meteorology]] and [[human physiology]] such as the [[heat index]] measuring the combined perceived effect of heat and [[humidity]], or the [[wind chill factor]] measuring the combined perceived effects of cold and wind.&lt;br /&gt;
&lt;br /&gt;
==Social sciences==&lt;br /&gt;
{{See also|Society for Quantitative Analysis of Behavior|Quantitative psychological research}}&lt;br /&gt;
&lt;br /&gt;
In the [[social sciences]], quantification is an integral part of [[economics]] and [[psychology]]. Both disciplines gather data—economics by [[empirical observation]] and psychology by [[experimentation]], and both use [[statistics|statistical techniques]] such as [[regression analysis]] to draw conclusions from it.&lt;br /&gt;
&lt;br /&gt;
In some instances a seemingly intangible property may be quantified by asking subjects to rate something on a [[Scale (social sciences)|scale]]—for example, a [[Happiness economics#Methodology|happiness scale]] or a [[Self-Perceived Quality of Life Scale|quality of life scale]]—or by the construction of a scale by the researcher, as with the [[index of economic freedom]]. In other cases, an unobservable variable may be quantified by replacing it with a [[proxy (statistics)|proxy variable]] with which it is highly correlated—for example, per capita [[gross domestic product]] is often used as a proxy for [[standard of living]] or [[quality of life]].&lt;br /&gt;
&lt;br /&gt;
Frequently in the use of regression, the presence or absence of a trait is quantified by employing a [[dummy variable (statistics)|dummy variable]], which takes on the value 1 in the presence of the trait or the value 0 in the absence of the trait.&lt;br /&gt;
&lt;br /&gt;
[[Quantitative linguistics]] is an area of [[linguistics]] that relies on quantification. For example,&amp;lt;ref&amp;gt;Bybee, Joan; Perkins, Revere; and Pagliuca, William. (1994) &#039;&#039;The Evolution of Grammar&#039;&#039;, Univ. of Chicago Press: ch. 4.&amp;lt;/ref&amp;gt; indices of [[grammaticalization]] of [[morpheme]]s, such as [[phonology|phonological]] shortness, dependence on surroundings, and fusion with the verb, have been developed and found to be significantly correlated across languages with stage of evolution of function of the morpheme.&lt;br /&gt;
&lt;br /&gt;
==Hard versus soft science==&lt;br /&gt;
The ease of quantification is one of the features used to distinguish [[hard and soft science]]s from each other. Hard sciences are often considered to be more scientific, rigorous, or accurate. In some [[social sciences]] such as [[sociology]], specific accurate data are difficult to obtain, either because laboratory conditions are not present or because the issues involved are conceptual but not directly quantifiable.{{facts|date=December 2013}}&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
{{Portal|Logic}}&lt;br /&gt;
*[[Indefinite pronoun]]&lt;br /&gt;
*[[Quantifier elimination]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
* [[Jon Barwise|Barwise, Jon]]; and [[John Etchemendy|Etchemendy, John]], 2000. &#039;&#039;Language Proof and Logic&#039;&#039;. CSLI (University of Chicago Press) and New York: Seven Bridges Press. A gentle introduction to [[first-order logic]] by two first-rate logicians.&lt;br /&gt;
* Crosby, Alfred W. (1996) &#039;&#039;The Measure of Reality: Quantification and Western Society, 1250-1600&#039;&#039;. Cambridge University Press.&lt;br /&gt;
* [[Gottlob Frege|Frege, Gottlob]], 1879. &#039;&#039;[[Begriffsschrift]]&#039;&#039;. Translated in [[Jean van Heijenoort]], 1967. &#039;&#039;From Frege to Gödel: A Source Book on Mathematical Logic, 1879-1931&#039;&#039;. Harvard University Press. The first appearance of quantification.&lt;br /&gt;
* [[David Hilbert|Hilbert, David]]; and [[Wilhelm Ackermann|Ackermann, Wilhelm]], 1950 (1928). &#039;&#039;[[Principles of Mathematical Logic]]&#039;&#039;. Chelsea. Translation of &#039;&#039;Grundzüge der theoretischen Logik&#039;&#039;. Springer-Verlag. The 1928 first edition is the first time quantification was consciously employed in the now-standard  manner, namely as binding variables ranging over some fixed domain of discourse. This is the defining aspect of [[first-order logic]].&lt;br /&gt;
* [[Charles Sanders Peirce|Peirce, C. S.]], 1885, &amp;quot;On the Algebra of Logic: A Contribution to the Philosophy of Notation, &#039;&#039;American Journal of Mathematics&#039;&#039;, Vol. 7, pp. 180–202. Reprinted in Kloesel, N. &#039;&#039;et al.&#039;&#039;, eds., 1993. &#039;&#039;Writings of C. S. Peirce, Vol. 5&#039;&#039;. Indiana University Press. The first appearance of quantification in anything like its present form.&lt;br /&gt;
* [[Hans Reichenbach|Reichenbach, Hans]], 1975 (1947). &#039;&#039;Elements of Symbolic Logic&#039;&#039;, Dover Publications. The quantifiers are discussed in chapters §18 &amp;quot;Binding of variables&amp;quot; through §30 &amp;quot;Derivations from Synthetic Premises&amp;quot;.&lt;br /&gt;
* Westerståhl, Dag, 2001, &amp;quot;Quantifiers,&amp;quot; in Goble, Lou, ed., &#039;&#039;The Blackwell Guide to Philosophical Logic&#039;&#039;. Blackwell.&lt;br /&gt;
* Wiese, Heike, 2003. &#039;&#039;Numbers, language, and the human mind&#039;&#039;. Cambridge University Press. ISBN 0-521-83182-2.&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
{{Wiktionary|quantification}}&lt;br /&gt;
* {{springer|title=Quantifier|id=p/q076260}}&lt;br /&gt;
* [[Stanford Encyclopedia of Philosophy]]:&lt;br /&gt;
** &amp;quot;[http://plato.stanford.edu/entries/logic-classical/ Classical Logic] &amp;amp;mdash; by Stewart Shapiro. Covers syntax, model theory, and metatheory for first order logic in the natural deduction style.&lt;br /&gt;
**&amp;quot;[http://plato.stanford.edu/entries/generalized-quantifiers/ Generalized quantifiers]&amp;quot; &amp;amp;mdash; by Dag Westerståhl.&lt;br /&gt;
* Peters, Stanley; Westerståhl, Dag (2002). &amp;quot;[http://www.stanford.edu/group/nasslli/courses/peters-wes/PWbookdraft2-3.pdf Quantifiers.]&amp;quot;&lt;br /&gt;
&lt;br /&gt;
{{Formal Fallacy}}&lt;br /&gt;
{{Logic}}&lt;br /&gt;
{{lexical categories|state=collapsed}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Logic]]&lt;br /&gt;
[[Category:Predicate logic]]&lt;br /&gt;
[[Category:Quantification]]&lt;br /&gt;
[[Category:Philosophical logic]]&lt;br /&gt;
[[Category:Semantics]]&lt;/div&gt;</summary>
		<author><name>131.111.184.10</name></author>
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		<title>Dirichlet density</title>
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		<updated>2013-12-06T01:17:04Z</updated>

		<summary type="html">&lt;p&gt;131.111.16.20: /* Definition */&lt;/p&gt;
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&lt;div&gt;{{Use dmy dates|date=August 2013}}&lt;br /&gt;
{{Unreferenced stub|auto=yes|date=December 2009}}&lt;br /&gt;
&#039;&#039;&#039;Charge-carrier density&#039;&#039;&#039; denotes the number of [[charge carrier]]s per [[volume]]. It is measured in m&amp;lt;sup&amp;gt;−3&amp;lt;/sup&amp;gt;. As any [[density]] it can depend on position.&lt;br /&gt;
It should not be confused with the [[charge density]], which is the number of charges per volume at a given energy.&lt;br /&gt;
&lt;br /&gt;
The carrier density is obtained by [[integral|integrating]] the charge density over the energy that the charges are allowed to have.&lt;br /&gt;
&lt;br /&gt;
Charge-carrier density is a [[particle density]], so [[integral|integrating]] it over a volume &amp;lt;math&amp;gt;V&amp;lt;/math&amp;gt; gives the number of charge carriers &amp;lt;math&amp;gt;N&amp;lt;/math&amp;gt; in that volume&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;N=\int_V n(\mathbf r) \,\mathrm{d}V&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
:&amp;lt;math&amp;gt;n(\mathbf r)&amp;lt;/math&amp;gt; is the position-dependent charge-carrier density.&lt;br /&gt;
&lt;br /&gt;
If the density does not depend on position and is instead equal to a constant &amp;lt;math&amp;gt;n_0&amp;lt;/math&amp;gt; this equation simplifies to&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;N=V\cdot n_0&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Charge-carrier densities involve equations concerning the [[electrical conductivity]] and related phenomena like the [[thermal conductivity]].&lt;br /&gt;
&lt;br /&gt;
==Measurement==&lt;br /&gt;
&lt;br /&gt;
The density of charge carriers can be determined in many cases using the [[Hall effect]], the voltage of which depends inversely on the density.&lt;br /&gt;
&lt;br /&gt;
Such measurements show that the density for silver is around 5.8·10&amp;lt;sup&amp;gt;28&amp;lt;/sup&amp;gt; m&amp;lt;sup&amp;gt;−3&amp;lt;/sup&amp;gt; or around 1.2 per atom.&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Charge Carrier Density}}&lt;br /&gt;
[[Category:Density]]&lt;br /&gt;
[[Category:Charge carriers]]&lt;br /&gt;
&lt;br /&gt;
{{Phys-stub}}&lt;/div&gt;</summary>
		<author><name>131.111.16.20</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Laplacian_of_the_indicator&amp;diff=28276</id>
		<title>Laplacian of the indicator</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Laplacian_of_the_indicator&amp;diff=28276"/>
		<updated>2013-12-03T11:03:36Z</updated>

		<summary type="html">&lt;p&gt;131.111.165.150: /* See also */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In mathematics, a &#039;&#039;&#039;local language&#039;&#039;&#039; is a [[formal language]] for which membership of a word in the language can be determined by looking at a &amp;quot;window&amp;quot; of length two.&amp;lt;ref name=Sal97&amp;gt;Salomaa (1981) p.97&amp;lt;/ref&amp;gt;  Equivalently, it is a language recognised by a [[local automaton]], a class of [[deterministic finite automaton]].&amp;lt;ref name=Law130&amp;gt;Lawson (2004) p.130&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Formally, we define a language &#039;&#039;L&#039;&#039; over an alphabet &#039;&#039;A&#039;&#039; to be &#039;&#039;local&#039;&#039; if there are subsets &#039;&#039;R&#039;&#039; and &#039;&#039;S&#039;&#039; of &#039;&#039;A&#039;&#039; and a subset &#039;&#039;F&#039;&#039; of &#039;&#039;A&#039;&#039;×&#039;&#039;A&#039;&#039; such that a word &#039;&#039;w&#039;&#039; is in &#039;&#039;L&#039;&#039; if and only if the first letter of &#039;&#039;w&#039;&#039; is in &#039;&#039;R&#039;&#039;, the last letter of &#039;&#039;w&#039;&#039; is in &#039;&#039;S&#039;&#039; and no factor of length 2 in &#039;&#039;w&#039;&#039; is in &#039;&#039;F&#039;&#039;.&amp;lt;ref name=Law129&amp;gt;Lawson (2004) p.129&amp;lt;/ref&amp;gt;  This corresponds to the [[regular expression]]&amp;lt;ref name=Sal97/&amp;gt;&amp;lt;ref name=Sak228&amp;gt;Sakarovitch (2009) p.228&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; (RA^* \cap A^*S) \setminus A^*FA^* \ . &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
More generally, a &#039;&#039;k&#039;&#039;-&#039;&#039;testable&#039;&#039; language &#039;&#039;L&#039;&#039; is one for which membership of a word &#039;&#039;w&#039;&#039; in &#039;&#039;L&#039;&#039; depends only on the prefix, suffix and the set of factors of &#039;&#039;w&#039;&#039; of length &#039;&#039;k&#039;&#039;; a language is &#039;&#039;locally testable&#039;&#039; if it is &#039;&#039;k&#039;&#039;-testable for some &#039;&#039;k&#039;&#039;.&amp;lt;ref&amp;gt;McNaughton &amp;amp; Papert (1971) p.14&amp;lt;/ref&amp;gt;  A local language is 2-testable.&amp;lt;ref name=Sal97/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Examples==&lt;br /&gt;
* Over the alphabet {&#039;&#039;a&#039;&#039;,&#039;&#039;b&#039;&#039;}&amp;lt;ref name=Sak228/&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; aa^*,\ \{ab\} \ . &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Properties==&lt;br /&gt;
* The family of local languages over &#039;&#039;A&#039;&#039; is closed under intersection and [[Kleene star]], but not complement, union or concatenation.&amp;lt;ref name=Sak228/&amp;gt;&lt;br /&gt;
* Every [[regular language]] not containing the empty string is the image of a local language under a [[strictly alphabetic morphism]].&amp;lt;ref name=Sal97/&amp;gt;&amp;lt;ref name=Law132&amp;gt;Lawson (2004) p.132&amp;lt;/ref&amp;gt;&amp;lt;ref name=MP18&amp;gt;McNaughton &amp;amp; Papert (1971) p.18&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
* {{cite book | last=Lawson | first=Mark V. | title=Finite automata | publisher=Chapman and Hall/CRC | year=2004 | isbn=1-58488-255-7 | zbl=1086.68074 }}&lt;br /&gt;
* {{cite book | last1=McNaughton | first1=Robert | last2 = Papert | first2=Seymour | author2-link=Seymour Papert | others=With an appendix by William Henneman | series=Research Monograph | volume=65 | year=1971 | title=Counter-free Automata | publisher=MIT Press | isbn=0-262-13076-9 | zbl=0232.94024 }}&lt;br /&gt;
* {{cite book | last=Sakarovitch | first=Jacques | title=Elements of automata theory | others=Translated from the French by Reuben Thomas | location=Cambridge | publisher=[[Cambridge University Press]] | year=2009 | isbn=978-0-521-84425-3 | zbl=1188.68177 }}&lt;br /&gt;
* {{cite book | first=Arto | last=Salomaa | authorlink=Arto Salomaa | title=Jewels of Formal Language Theory | publisher=Pitman Publishing | isbn=0-273-08522-0 | year=1981 | zbl=0487.68064 }}&lt;br /&gt;
&lt;br /&gt;
{{algebra-stub}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Semigroup theory]]&lt;br /&gt;
[[Category:Formal languages]]&lt;br /&gt;
[[Category:Combinatorics on words]]&lt;/div&gt;</summary>
		<author><name>131.111.165.150</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Double_layer_potential&amp;diff=24291</id>
		<title>Double layer potential</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Double_layer_potential&amp;diff=24291"/>
		<updated>2013-12-03T11:03:22Z</updated>

		<summary type="html">&lt;p&gt;131.111.165.150: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[condensed matter physics]], the &#039;&#039;&#039;dynamic structure factor&#039;&#039;&#039; is a mathematical function that contains information about inter-particle correlations and their time evolution. It is a generalization of the [[structure factor]] which considers correlations in both space &#039;&#039;and&#039;&#039; time. Experimentally, it can be accessed most directly by [[inelastic neutron scattering]].&lt;br /&gt;
&lt;br /&gt;
The dynamic structure factor is most often denoted &amp;lt;math&amp;gt;S(\vec{k},\omega)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;\vec{k}&amp;lt;/math&amp;gt; (sometimes &amp;lt;math&amp;gt;\vec{q}&amp;lt;/math&amp;gt;) is a wave vector (or wave number for isotropic materials), and &amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt; a frequency (sometimes stated as energy, &amp;lt;math&amp;gt;\hbar\omega&amp;lt;/math&amp;gt;). It is defined as:&amp;lt;ref name = &amp;quot;theoryliquids&amp;quot;&amp;gt;&lt;br /&gt;
{{cite book &lt;br /&gt;
 |first=J.P. |last=Hansen |first2=I.R. |last2=McDonald&lt;br /&gt;
 |title=Theory of Simple Liquids&lt;br /&gt;
 |publisher=[[Academic Press]]&lt;br /&gt;
 |page=&lt;br /&gt;
 |year=1986&lt;br /&gt;
 |isbn=&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
:&amp;lt;math&amp;gt;S(\vec{k},\omega) \equiv \frac{1}{2\pi}\int_{-\infty}^{\infty} F(\vec{k},t)\mbox{exp}(i\omega t) dt&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Here &amp;lt;math&amp;gt;F(\vec{k},t)&amp;lt;/math&amp;gt;, is called the &#039;&#039;&#039;intermediate scattering function&#039;&#039;&#039; and can be measured by [[neutron spin echo]] spectroscopy. The intermediate scattering function is the spatial [[Fourier transform]] of the &#039;&#039;&#039;van Hove function&#039;&#039;&#039; &amp;lt;math&amp;gt;G(\vec{r},t)&amp;lt;/math&amp;gt;:&amp;lt;ref&amp;gt;{{cite journal&lt;br /&gt;
 |last=van Hove |first=L.&lt;br /&gt;
 |title=Correlations in Space and Time and Born Approximation Scattering in Systems of Interacting Particles&lt;br /&gt;
 |volume=95 |issue=1 |page=249&lt;br /&gt;
 |journal=[[Physical Review]]&lt;br /&gt;
 |year=1954&lt;br /&gt;
 |doi=10.1103/PhysRev.95.249&lt;br /&gt;
|bibcode = 1954PhRv...95..249V }}&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;G. Vineyard, &amp;quot;Scattering of Slow Neutrons by a Liquid&amp;quot;, Phys. Rev. 110, 999-1010&lt;br /&gt;
(1958).&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;F(\vec{k},t) \equiv \int G(\vec{r},t)\exp (-i\vec{k}\cdot\vec{r}) d\vec{r}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus we see that the dynamical structure factor is the spatial &#039;&#039;and&#039;&#039; temporal  Fourier transform of [[Leon van Hove|van Hove]]&#039;s time-dependent pair correlation function. It can be shown (see below), that the intermediate scattering function is the correlation function of the Fourier components of the density &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt;: &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;F(\vec{k},t) = \frac{1}{N}\langle \rho_{\vec{k}}(t)\rho_{-\vec{k}} \rangle&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The dynamic structure is exactly what is probed in coherent inelastic neutron scattering. The [[differential cross section]] is : &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d^2 \sigma}{d\Omega d\omega} = a^2\left(\frac{E_f}{E_i}\right)^{1/2} S(\vec{k},\omega) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;a&amp;lt;/math&amp;gt; is the [[scattering length]]. &lt;br /&gt;
&lt;br /&gt;
==The van Hove Function==&lt;br /&gt;
The van Hove Function for a spatially uniform system containing &amp;lt;math&amp;gt;N&amp;lt;/math&amp;gt; point particles is defined as:&amp;lt;ref name = &amp;quot;theoryliquids&amp;quot;/&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;G(\vec{r},t) = \langle \frac{1}{N} \int \sum_{i=1}^{N}\sum_{j=1}^N \delta[\vec{r}&#039;+\vec{r}-\vec{r}_j]\delta[\vec{r}&#039;-\vec{r}_i(0)] d\vec{r}&#039; \rangle&amp;lt;/math&amp;gt;&lt;br /&gt;
It can be rewritten as: &lt;br /&gt;
:&amp;lt;math&amp;gt;G(\vec{r},t) = \langle \frac{1}{N}\int \rho(\vec{r}&#039;+\vec{r},t)\rho(\vec{r}&#039;,0) d\vec{r}&#039;\rangle &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In an isotropic sample (with scalar &#039;&#039;r&#039;&#039;), &#039;&#039;G(r,t)&#039;&#039; is a time dependent  [[radial distribution function]].&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
== Further reading ==&lt;br /&gt;
*&lt;br /&gt;
&lt;br /&gt;
[[Category:Condensed matter physics]]&lt;br /&gt;
[[Category:Neutron scattering]]&lt;/div&gt;</summary>
		<author><name>131.111.165.150</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Wick_rotation&amp;diff=3704</id>
		<title>Wick rotation</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Wick_rotation&amp;diff=3704"/>
		<updated>2013-11-26T16:50:43Z</updated>

		<summary type="html">&lt;p&gt;131.111.16.20: /* Overview */  changed sign of Wick rotation. It is t-&amp;gt;-i\tau&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{technical|date=May 2013}}&lt;br /&gt;
{{DISPLAYTITLE:E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; (mathematics)}}&lt;br /&gt;
{{Group theory sidebar |Topological}}&lt;br /&gt;
{{Lie groups |Simple}}&lt;br /&gt;
&lt;br /&gt;
In [[mathematics]], &#039;&#039;&#039;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039; is the name of some closely related [[Lie group]]s, linear [[algebraic group]]s or their [[Lie algebra]]s &amp;lt;math&amp;gt;\mathfrak{e}_6&amp;lt;/math&amp;gt;, all of which have dimension 78; the same notation E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; is used for the corresponding [[root lattice]], which has [[Rank of a Lie group|rank]]&amp;amp;nbsp;6.  The designation E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; comes from the Cartan–Killing classification of the complex [[simple Lie algebra]]s, which fall into four infinite series labeled A&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt;, B&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt;, C&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt;, D&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt;, and [[Exceptional simple Lie group|five exceptional cases]] labeled E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, [[E7 (mathematics)|E&amp;lt;sub&amp;gt;7&amp;lt;/sub&amp;gt;]], [[E8 (mathematics)|E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt;]], [[F4 (mathematics)|F&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;]], and [[G2 (mathematics)|G&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]. The E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; algebra is thus one of the five exceptional cases.&lt;br /&gt;
&lt;br /&gt;
The fundamental group of the complex form, compact real form, or any algebraic version of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; is the [[cyclic group]] &#039;&#039;&#039;Z&#039;&#039;&#039;/3&#039;&#039;&#039;Z&#039;&#039;&#039;, and its [[outer automorphism group]] is the cyclic group &#039;&#039;&#039;Z&#039;&#039;&#039;/2&#039;&#039;&#039;Z&#039;&#039;&#039;. Its [[fundamental representation]] is 27-dimensional (complex), and a basis is given by the [[27 lines on a cubic surface]]. The [[dual representation]], which is inequivalent, is also 27-dimensional.&lt;br /&gt;
&lt;br /&gt;
In [[particle physics]], E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; plays a role in some [[grand unified theory|grand unified theories]].&lt;br /&gt;
&lt;br /&gt;
==Real and complex forms==&lt;br /&gt;
There is a unique complex Lie algebra of type E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, corresponding to a complex group of complex dimension 78. The complex adjoint Lie group E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; of [[complex dimension]] 78 can be considered as a simple real Lie group of real dimension 156. This has fundamental group &#039;&#039;&#039;Z&#039;&#039;&#039;/3&#039;&#039;&#039;Z&#039;&#039;&#039;, has maximal [[Compact space|compact]] subgroup the compact form (see below) of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, and has an outer automorphism group non-cyclic of order 4 generated by complex conjugation and by the outer automorphism which already exists as a complex automorphism.&lt;br /&gt;
&lt;br /&gt;
As well as the complex Lie group of type E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, there are five real forms of the Lie algebra, and correspondingly five real forms of the group with trivial center (all of which have an algebraic double cover, and three of which have further non-algebraic covers, giving further real forms), all of real dimension 78, as follows:&lt;br /&gt;
&lt;br /&gt;
*The compact form (which is usually the one meant if no other information is given), which has fundamental group &#039;&#039;&#039;Z&#039;&#039;&#039;/3&#039;&#039;&#039;Z&#039;&#039;&#039; and outer automorphism group &#039;&#039;&#039;Z&#039;&#039;&#039;/2&#039;&#039;&#039;Z&#039;&#039;&#039;.&lt;br /&gt;
*The split form, EI (or E&amp;lt;sub&amp;gt;6(6)&amp;lt;/sub&amp;gt;), which has maximal compact subgroup Sp(4)/(±1), fundamental group of order 2 and outer automorphism group of order 2.&lt;br /&gt;
*The quasi-split form EII (or E&amp;lt;sub&amp;gt;6(2)&amp;lt;/sub&amp;gt;), which has maximal compact subgroup SU(2) × SU(6)/(center), fundamental group cyclic of order 6 and outer automorphism group of order 2.&lt;br /&gt;
*EIII (or E&amp;lt;sub&amp;gt;6(-14)&amp;lt;/sub&amp;gt;), which has maximal compact subgroup SO(2) × Spin(10)/(center), fundamental group &#039;&#039;&#039;Z&#039;&#039;&#039; and trivial outer automorphism group.&lt;br /&gt;
*EIV (or E&amp;lt;sub&amp;gt;6(-26)&amp;lt;/sub&amp;gt;), which has maximal compact subgroup F&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;, trivial fundamental group cyclic and outer automorphism group of order 2.&lt;br /&gt;
&lt;br /&gt;
The EIV form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; is the group of collineations (line-preserving transformations) of the [[octonionic projective plane]] &#039;&#039;&#039;OP&#039;&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;.&amp;lt;ref&amp;gt;{{Citation | last1=Rosenfeld | first1=Boris | title=Geometry of Lie Groups | year=1997 }} (theorem 7.4 on page 335, and following paragraph).&amp;lt;/ref&amp;gt; It is also the group of determinant-preserving linear transformations of the exceptional [[Jordan algebra]]. The exceptional Jordan algebra is 27-dimensional, which explains why the compact real form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; has a 27-dimensional complex representation. The compact real form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; is the [[isometry group]] of a 32-dimensional [[Riemannian manifold]] known as the &#039;bioctonionic projective plane&#039;; similar constructions for E&amp;lt;sub&amp;gt;7&amp;lt;/sub&amp;gt; and E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt; are known as the [[Rosenfeld projective plane]]s, and are part of the [[Freudenthal magic square]].&lt;br /&gt;
&lt;br /&gt;
==E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; as an algebraic group==&lt;br /&gt;
By means of a [[Chevalley basis]] for the Lie algebra, one can define E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; as a linear algebraic group over the integers and, consequently, over any commutative ring and in particular over any field: this defines the so-called split (sometimes also known as “untwisted”) adjoint form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;. Over an algebraically closed field, this and its triple cover are the only forms; however, over other fields, there are often many other forms, or “twists” of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, which are classified in the general framework of [[Galois cohomology]] (over a [[perfect field]] &#039;&#039;k&#039;&#039;) by the set &#039;&#039;H&#039;&#039;&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;(&#039;&#039;k&#039;&#039;, Aut(E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;)) which, because the Dynkin diagram of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; (see [[#Dynkin diagram|below]]) has automorphism group &#039;&#039;&#039;Z&#039;&#039;&#039;/2&#039;&#039;&#039;Z&#039;&#039;&#039;, maps to &#039;&#039;H&#039;&#039;&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;(&#039;&#039;k&#039;&#039;, &#039;&#039;&#039;Z&#039;&#039;&#039;/2&#039;&#039;&#039;Z&#039;&#039;&#039;) = Hom (Gal(&#039;&#039;k&#039;&#039;), &#039;&#039;&#039;Z&#039;&#039;&#039;/2&#039;&#039;&#039;Z&#039;&#039;&#039;) with kernel &#039;&#039;H&#039;&#039;&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;(&#039;&#039;k&#039;&#039;, E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;).&amp;lt;ref&amp;gt;{{cite book | last1=Платонов | first1=Владимир П. | last2=Рапинчук | first2=Андрей С. | title=Алгебраические группы и теория чисел | year=1991 | publisher=Наука | isbn=5-02-014191-7 }} (English translation: {{cite book | last1=Platonov | first1=Vladimir P. | last2=Rapinchuk | first2=Andrei S. | title=Algebraic groups and number theory | year=1994 | publisher=Academic Press | isbn=0-12-558180-7 }}), §2.2.4&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Over the field of real numbers, the real component of the identity of these algebraically twisted forms of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; coincide with the three real Lie groups mentioned [[#Real and complex forms|above]], but with a subtlety concerning the fundamental group: all adjoint forms of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; have fundamental group &#039;&#039;&#039;Z&#039;&#039;&#039;/3&#039;&#039;&#039;Z&#039;&#039;&#039; in the sense of algebraic geometry, with Galois action as on the third roots of unity; this means that they admit exactly one triple cover (which may be trivial on the real points); the further non-compact real Lie group forms of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; are therefore not algebraic and admit no faithful finite-dimensional representations.  The compact real form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; as well as the noncompact forms EI=E&amp;lt;sub&amp;gt;6(6)&amp;lt;/sub&amp;gt; and EIV=E&amp;lt;sub&amp;gt;6(-26)&amp;lt;/sub&amp;gt; are said to be &#039;&#039;inner&#039;&#039; or of type &amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; meaning that their class lies in &#039;&#039;H&#039;&#039;&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;(&#039;&#039;k&#039;&#039;, E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;) or that complex conjugation induces the trivial automorphism on the Dynkin diagram, whereas the other two real forms are said to be &#039;&#039;outer&#039;&#039; or of type &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Over finite fields, the [[Lang–Steinberg theorem]] implies that &#039;&#039;H&#039;&#039;&amp;lt;sup&amp;gt;1&amp;lt;/sup&amp;gt;(&#039;&#039;k&#039;&#039;, E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;) = 0, meaning that E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; has exactly one twisted form, known as &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;: see [[#Chevalley and Steinberg groups of type E6 and 2E6|below]].&lt;br /&gt;
&lt;br /&gt;
== Algebra ==&lt;br /&gt;
&lt;br /&gt;
===Dynkin diagram===&lt;br /&gt;
The [[Dynkin diagram]] for E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; is given by [[Image:Dynkin diagram E6.png|120px|Dynkin diagram of E 6]], {{Dynkin2|node|3|node|3|branch|3|node|3|node}} or sometimes positioned like this {{Dynkin|nodes|3s|nodes|loop2|3|node}}.&lt;br /&gt;
&lt;br /&gt;
=== Roots of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; ===&lt;br /&gt;
[[File:Gosset 1 22 polytope.svg|thumb|300px|The 72 vertices of the [[1 22 polytope|1&amp;lt;sub&amp;gt;22&amp;lt;/sub&amp;gt;]] polytope represent the root vectors of the E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, as shown in this [[Coxeter plane]] projection.&amp;lt;p&amp;gt;[[Coxeter-Dynkin diagram]]: {{CDD|node_1|3|node|split1|nodes|3ab|nodes}}]]&lt;br /&gt;
&lt;br /&gt;
Although they [[Linear span|span]] a six-dimensional space, it is much more symmetrical to consider them as [[Vector space|vectors]] in a six-dimensional subspace of a nine-dimensional space.&lt;br /&gt;
:(1,&amp;amp;minus;1,0;0,0,0;0,0,0), (&amp;amp;minus;1,1,0;0,0,0;0,0,0),&lt;br /&gt;
:(&amp;amp;minus;1,0,1;0,0,0;0,0,0), (1,0,&amp;amp;minus;1;0,0,0;0,0,0),&lt;br /&gt;
:(0,1,&amp;amp;minus;1;0,0,0;0,0,0), (0,&amp;amp;minus;1,1;0,0,0;0,0,0),&lt;br /&gt;
:(0,0,0;1,&amp;amp;minus;1,0;0,0,0), (0,0,0;&amp;amp;minus;1,1,0;0,0,0),&lt;br /&gt;
:(0,0,0;&amp;amp;minus;1,0,1;0,0,0), (0,0,0;1,0,&amp;amp;minus;1;0,0,0),&lt;br /&gt;
:(0,0,0;0,1,&amp;amp;minus;1;0,0,0), (0,0,0;0,&amp;amp;minus;1,1;0,0,0),&lt;br /&gt;
:(0,0,0;0,0,0;1,&amp;amp;minus;1,0), (0,0,0;0,0,0;&amp;amp;minus;1,1,0),&lt;br /&gt;
:(0,0,0;0,0,0;&amp;amp;minus;1,0,1), (0,0,0;0,0,0;1,0,&amp;amp;minus;1),&lt;br /&gt;
:(0,0,0;0,0,0;0,1,&amp;amp;minus;1), (0,0,0;0,0,0;0,&amp;amp;minus;1,1),&lt;br /&gt;
&lt;br /&gt;
All 27 combinations of &amp;lt;math&amp;gt;(\bold{3};\bold{3};\bold{3})&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;\bold{3}&amp;lt;/math&amp;gt; is one of &amp;lt;math&amp;gt;\left(\frac{2}{3}, -\frac{1}{3}, -\frac{1}{3}\right),\ \left( -\frac{1}{3}, \frac{2}{3}, -\frac{1}{3}\right),\  \left( -\frac{1}{3}, -\frac{1}{3}, \frac{2}{3} \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
All 27 combinations of &amp;lt;math&amp;gt;(\bar{\bold{3}};\bar{\bold{3}};\bar{\bold{3}})&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;\bar{\bold{3}}&amp;lt;/math&amp;gt; is one of &amp;lt;math&amp;gt;\left(-\frac{2}{3},\frac{1}{3},\frac{1}{3}\right),\ \left(\frac{1}{3}, -\frac{2}{3}, \frac{1}{3} \right),\ \left( \frac{1}{3}, \frac{1}{3}, -\frac{2}{3} \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Simple roots&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
:(0,0,0;0,0,0;0,1,&amp;amp;minus;1)&lt;br /&gt;
&lt;br /&gt;
:(0,0,0;0,0,0;1,&amp;amp;minus;1,0)&lt;br /&gt;
&lt;br /&gt;
:(0,0,0;0,1,&amp;amp;minus;1;0,0,0)&lt;br /&gt;
&lt;br /&gt;
:(0,0,0;1,&amp;amp;minus;1,0;0,0,0)&lt;br /&gt;
&lt;br /&gt;
:(0,1,&amp;amp;minus;1;0,0,0;0,0,0)&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left(\frac{1}{3},-\frac{2}{3},\frac{1}{3};-\frac{2}{3},\frac{1}{3},\frac{1}{3};-\frac{2}{3},\frac{1}{3},\frac{1}{3}\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Image:E6Coxeter.svg|thumb|300px|Graph of E6 as a subgroup of E8 projected into the Coxeter plane]]&lt;br /&gt;
[[File:E6HassePoset.svg|thumb|300px|[[Hasse diagram]] of E6 [[Root system#The root poset|root poset]] with edge labels identifying added simple root position]]&lt;br /&gt;
&lt;br /&gt;
==== An alternative description ====&lt;br /&gt;
An alternative (6-dimensional) description of the root system, which is useful in considering E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; × SU(3) as a [[E8 (mathematics)#Subgroups|subgroup of]] E&amp;lt;sub&amp;gt;8&amp;lt;/sub&amp;gt;, is the following:&lt;br /&gt;
&lt;br /&gt;
All &amp;lt;math&amp;gt;4\times\begin{pmatrix}5\\2\end{pmatrix}&amp;lt;/math&amp;gt; permutations of&lt;br /&gt;
:&amp;lt;math&amp;gt;(\pm1,\pm1,0,0,0,0)&amp;lt;/math&amp;gt; preserving the zero at the last entry,&lt;br /&gt;
&lt;br /&gt;
and all of the following roots with an odd number of plus signs&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left(\pm{1\over 2},\pm{1\over 2},\pm{1\over 2},\pm{1\over 2},\pm{1\over 2},\pm{\sqrt{3}\over 2}\right).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus the 78 generators consist of the following subalgebras:&lt;br /&gt;
: A 45-dimensional SO(10) subalgebra, including the above &amp;lt;math&amp;gt;4\times\begin{pmatrix}5\\2\end{pmatrix}&amp;lt;/math&amp;gt; generators plus the five [[Cartan subalgebra|Cartan generator]]s corresponding to the first five entries.&lt;br /&gt;
: Two 16-dimensional subalgebras that transform as a [[Weyl spinor]] of &amp;lt;math&amp;gt;\operatorname{spin}(10)&amp;lt;/math&amp;gt; and its complex conjugate. These have a non-zero last entry.&lt;br /&gt;
: 1 generator which is their chirality generator, and is the sixth [[Cartan subalgebra|Cartan generator]].&lt;br /&gt;
&lt;br /&gt;
One choice of [[Simple root (root system)|simple root]]s for E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, index as [[File:DynkinE6.svg|120px]], is given by the rows of the following matrix:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left [\begin{smallmatrix}&lt;br /&gt;
1&amp;amp;-1&amp;amp;0&amp;amp;0&amp;amp;0&amp;amp;0 \\&lt;br /&gt;
0&amp;amp;1&amp;amp;-1&amp;amp;0&amp;amp;0&amp;amp;0 \\&lt;br /&gt;
0&amp;amp;0&amp;amp;1&amp;amp;-1&amp;amp;0&amp;amp;0 \\&lt;br /&gt;
0&amp;amp;0&amp;amp;0&amp;amp;1&amp;amp;1&amp;amp;0 \\&lt;br /&gt;
-\frac{1}{2}&amp;amp;-\frac{1}{2}&amp;amp;-\frac{1}{2}&amp;amp;-\frac{1}{2}&amp;amp;-\frac{1}{2}&amp;amp;\frac{\sqrt{3}}{2}\\&lt;br /&gt;
0&amp;amp;0&amp;amp;0&amp;amp;1&amp;amp;-1&amp;amp;0 \\&lt;br /&gt;
\end{smallmatrix}\right ]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
we have ordered them so that their corresponding nodes in the [[Dynkin diagram]] are ordered from left to right (in the diagram depicted above) with the side node last.&lt;br /&gt;
&lt;br /&gt;
=== Weyl group ===&lt;br /&gt;
The [[Weyl group]] of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; is of order 51840: it is the [[automorphism]] group of the unique [[simple group]] of order 25920 (which can be described as any of: PSU&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;(2), PSΩ&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&amp;lt;sup&amp;gt;−&amp;lt;/sup&amp;gt;(2), PSp&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;(3) or PSΩ&amp;lt;sub&amp;gt;5&amp;lt;/sub&amp;gt;(3)).&amp;lt;ref&amp;gt;{{cite book |last1=Conway |first1=John Horton |authorlink1=John Horton Conway |last2=Curtis |first2=Robert Turner |last3=Norton |first3=Simon Phillips |authorlink3=Simon P. Norton |last4=Parker |first4=Richard A |authorlink4=Richard A. Parker |last5=Wilson |first5=Robert Arnott |authorlink5=Robert Arnott Wilson |title=[[ATLAS of Finite Groups|Atlas of Finite Groups]]: Maximal Subgroups and Ordinary Characters for Simple Groups |year=1985 |month= |publisher=Oxford University Press |isbn=0-19-853199-0 |page=26 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Cartan matrix ===&lt;br /&gt;
:&amp;lt;math&amp;gt;\left [\begin{smallmatrix}&lt;br /&gt;
2&amp;amp;-1&amp;amp;0&amp;amp;0&amp;amp;0&amp;amp;0\\&lt;br /&gt;
-1&amp;amp;2&amp;amp;-1&amp;amp;0&amp;amp;0&amp;amp;0\\&lt;br /&gt;
0&amp;amp;-1&amp;amp;2&amp;amp;-1&amp;amp;0&amp;amp;-1\\&lt;br /&gt;
0&amp;amp;0&amp;amp;-1&amp;amp;2&amp;amp;-1&amp;amp;0\\&lt;br /&gt;
0&amp;amp;0&amp;amp;0&amp;amp;-1&amp;amp;2&amp;amp;0\\&lt;br /&gt;
0&amp;amp;0&amp;amp;-1&amp;amp;0&amp;amp;0&amp;amp;2&lt;br /&gt;
\end{smallmatrix}\right ]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Important subalgebras and representations==&lt;br /&gt;
The Lie algebra E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; has an F&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; subalgebra, which is the fixed subalgebra of an outer automorphism, and an SU(3) × SU(3) × SU(3) subalgebra. Other maximal subalgebras which have an importance in physics (see below) and can be read off the Dynkin diagram, are the algebras of SO(10) × U(1) and SU(6) × SU(2).&lt;br /&gt;
&lt;br /&gt;
In addition to the 78-dimensional adjoint representation, there  are two dual [[E8 (mathematics)#Subgroups|27-dimensional &amp;quot;vector&amp;quot; representation]]s.&lt;br /&gt;
&lt;br /&gt;
The characters of finite dimensional representations of the real and complex Lie algebras and Lie groups are all given by the [[Weyl character formula]].  The dimensions of the smallest irreducible representations are {{OEIS|id=A121737}}:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;u&amp;gt;1&amp;lt;/u&amp;gt;, 27 (twice), &amp;lt;u&amp;gt;78&amp;lt;/u&amp;gt;, 351 (four times), &amp;lt;u&amp;gt;650&amp;lt;/u&amp;gt;, 1728 (twice), &amp;lt;u&amp;gt;2430&amp;lt;/u&amp;gt;, &amp;lt;u&amp;gt;2925&amp;lt;/u&amp;gt;, &amp;lt;u&amp;gt;3003 (twice)&amp;lt;/u&amp;gt;, &amp;lt;u&amp;gt;5824 (twice)&amp;lt;/u&amp;gt;, 7371 (twice), 7722 (twice), 17550 (twice), 19305 (four times), 34398 (twice), &amp;lt;u&amp;gt;34749&amp;lt;/u&amp;gt;, &amp;lt;u&amp;gt;43758&amp;lt;/u&amp;gt;, 46332 (twice), 51975 (twice), 54054 (twice), 61425 (twice), &amp;lt;u&amp;gt;70070&amp;lt;/u&amp;gt;, &amp;lt;u&amp;gt;78975 (twice)&amp;lt;/u&amp;gt;, &amp;lt;u&amp;gt;85293&amp;lt;/u&amp;gt;, 100386 (twice), &amp;lt;u&amp;gt;105600&amp;lt;/u&amp;gt;, 112320 (twice), &amp;lt;u&amp;gt;146432 (twice)&amp;lt;/u&amp;gt;, &amp;lt;u&amp;gt;252252 (twice)&amp;lt;/u&amp;gt;, 314496 (twice), 359424 (four times), &amp;lt;u&amp;gt;371800 (twice)&amp;lt;/u&amp;gt;, 386100 (twice), 393822 (twice), 412776 (twice), &amp;lt;u&amp;gt;442442 (twice)&amp;lt;/u&amp;gt;&amp;amp;hellip;&lt;br /&gt;
&lt;br /&gt;
The underlined terms in the sequence above are the dimensions of those irreducible representations possessed by the adjoint form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; (equivalently, those whose weights belong to the root lattice of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;), whereas the full sequence gives the dimensions of the irreducible representations of the simply connected form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The symmetry of the Dynkin diagram of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; explains why many dimensions occur twice, the corresponding representations being related by the non-trivial outer automorphism; however, there are sometimes even more representations than this, such as four of dimension 351, two of which are fundamental and two of which are not.&lt;br /&gt;
&lt;br /&gt;
The [[fundamental representation]]s have dimensions 27, 351, 2925, 351, 27 and 78 (corresponding to the seven nodes in the [[#Dynkin diagram|Dynkin diagram]] in the order chosen for the [[#Cartan matrix|Cartan matrix]] above, i.e., the nodes are read in the five-node chain first, with the last node being connected to the middle one).&lt;br /&gt;
&lt;br /&gt;
==E6 polytope==&lt;br /&gt;
The &#039;&#039;&#039;[[E6 polytope|E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; polytope]]&#039;&#039;&#039; is the [[convex hull]] of the roots of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;. It therefore exists in 6 dimensions; its [[symmetry group]] contains the [[Coxeter group]] for E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; as an [[Index of a subgroup|index]] 2 subgroup.&lt;br /&gt;
&lt;br /&gt;
==Chevalley and Steinberg groups of type E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; and &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
{{main|²E₆}}&lt;br /&gt;
&lt;br /&gt;
The groups of type &#039;&#039;E&#039;&#039;&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; over arbitrary fields (in particular finite fields) were introduced by {{harvs|txt|last=Dickson|year1=1901|year2=1908}}.&lt;br /&gt;
&lt;br /&gt;
The points over a [[finite field]] with &#039;&#039;q&#039;&#039; elements of the (split) algebraic group E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; (see [[#E6 as an algebraic group|above]]), whether of the adjoint (centerless) or simply connected form (its algebraic universal cover), give a finite [[Group of Lie type|Chevalley group]].  This is closely connected to the group written E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;), however there is ambiguity in this notation, which can stand for several things:&lt;br /&gt;
* the finite group consisting of the points over &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt; of the simply connected form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; (for clarity, this can be written E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) or more rarely &amp;lt;math&amp;gt;\tilde E_6(q)&amp;lt;/math&amp;gt; and is known as the &amp;quot;universal&amp;quot; Chevalley group of type E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; over &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt;),&lt;br /&gt;
* (rarely) the finite group consisting of the points over &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt; of the adjoint form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; (for clarity, this can be written E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;), and is known as the &amp;quot;adjoint&amp;quot; Chevalley group of type E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; over &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt;), or&lt;br /&gt;
* the finite group which is the image of the natural map from the former to the latter: this is what will be denoted by E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) in the following, as is most common in texts dealing with finite groups.&lt;br /&gt;
&lt;br /&gt;
From the finite group perspective, the relation between these three groups, which is quite analogous to that between SL(&#039;&#039;n,q&#039;&#039;), PGL(&#039;&#039;n,q&#039;&#039;) and PSL(&#039;&#039;n,q&#039;&#039;), can be summarized as follows: E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is simple for any &#039;&#039;q&#039;&#039;, E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is its [[Schur multiplier|Schur cover]], and E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) lies in its automorphism group; furthermore, when &#039;&#039;q&#039;&#039;−1 is not divisible by 3, all three coincide, and otherwise (when &#039;&#039;q&#039;&#039; is congruent to 1 mod 3), the Schur multiplier of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is 3 and E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is of index 3 in E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;), which explains why E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) and E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) are often written as 3·E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) and E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;)·3. From the algebraic group perspective, it is less common for E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) to refer to the finite simple group, because the latter is not in a natural way the set of points of an algebraic group over &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt; unlike E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) and E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;).&lt;br /&gt;
&lt;br /&gt;
Beyond this “split” (or “untwisted”) form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, there is also one other form of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; over the finite field &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt;, known as &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, which is obtained by twisting by the non-trivial automorphism of the Dynkin diagram of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;. Concretely, &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;), which is known as a Steinberg group, can be seen as the subgroup of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;) fixed by the composition of the non-trivial diagram automorphism and the non-trivial field automorphism of &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt;.  Twisting does not change the fact that the algebraic fundamental group of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt; is &#039;&#039;&#039;Z&#039;&#039;&#039;/3&#039;&#039;&#039;Z&#039;&#039;&#039;, but it does change those &#039;&#039;q&#039;&#039; for which the covering of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt; by &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt; is non-trivial on the &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt;-points.  Precisely: &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is a covering of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;), and &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) lies in its automorphism group; when &#039;&#039;q&#039;&#039;+1 is not divisible by 3, all three coincide, and otherwise (when &#039;&#039;q&#039;&#039; is congruent to 2 mod 3), the degree of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) over &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is 3 and &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is of index 3 in &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;), which explains why &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) and &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) are often written as 3·&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) and &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;)·3.&lt;br /&gt;
&lt;br /&gt;
Two notational issues should be raised concerning the groups &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;).  One is that this is sometimes written &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;), a notation which has the advantage of transposing more easily to the Suzuki and Ree groups, but the disadvantage of deviating from the notation for the &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt;-points of an algebraic group.  Another is that whereas &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) and &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) are the &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;/sub&amp;gt;-points of an algebraic group, the group in question also depends on &#039;&#039;q&#039;&#039; (e.g., the points over &#039;&#039;&#039;F&#039;&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;q&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;/sub&amp;gt; of the same group are the untwisted E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;) and E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;)).&lt;br /&gt;
&lt;br /&gt;
The groups E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) and &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) are simple for any &#039;&#039;q&#039;&#039;,&amp;lt;ref&amp;gt;{{cite book | first=Roger W. | last=Carter | title=Simple Groups of Lie Type | authorlink=Roger Carter (mathematician) | publisher=John Wiley &amp;amp;amp; Sons | series=Wiley Classics Library | isbn=0-471-50683-4 | year=1989 }}&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;{{cite book | first=Robert A. | last=Wilson | title=The Finite Simple Groups | authorlink=Robert Arnott Wilson | publisher=[[Springer-Verlag]] | series=[[Graduate Texts in Mathematics]] | volume=251 | isbn=1-84800-987-9 | year=2009 }}&amp;lt;/ref&amp;gt; and constitute two of the infinite families in the [[classification of finite simple groups]]. Their order is given by the following formula {{OEIS|id=A008872}}:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;|E_6 (q)| = \frac{1}{\mathrm{gcd}(3,q-1)}q^{36}(q^{12}-1)(q^9-1)(q^8-1)(q^6-1)(q^5-1)(q^2-1)&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;|{}^2\!E_6 (q)| = \frac{1}{\mathrm{gcd}(3,q+1)}q^{36}(q^{12}-1)(q^9+1)(q^8-1)(q^6-1)(q^5+1)(q^2-1)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{OEIS|id=A008916}}. The order of E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) or E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) (both are equal) can be obtained by removing the dividing factor gcd(3,&#039;&#039;q&#039;&#039;−1) from the first formula {{OEIS|id=A008871}}, and the order of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) or &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) (both are equal) can be obtained by removing the dividing factor gcd(3,&#039;&#039;q&#039;&#039;+1) from the second {{OEIS|id=A008915}}.&lt;br /&gt;
&lt;br /&gt;
The Schur multiplier of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is always gcd(3,&#039;&#039;q&#039;&#039;−1) (i.e., E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is its Schur cover). The Schur multiplier of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is gcd(3,&#039;&#039;q&#039;&#039;+1) (i.e., &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,sc&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is its Schur cover) outside of the exceptional case &#039;&#039;q&#039;&#039;=2 where it is 2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;·3 (i.e., there is an additional 2&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;-fold cover).  The outer automorphism group of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is the product of the diagonal automorphism group &#039;&#039;&#039;Z&#039;&#039;&#039;/gcd(3,&#039;&#039;q&#039;&#039;−1)&#039;&#039;&#039;Z&#039;&#039;&#039; (given by the action of E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;)), the group &#039;&#039;&#039;Z&#039;&#039;&#039;/2&#039;&#039;&#039;Z&#039;&#039;&#039; of diagram automorphisms, and the group of field automorphisms (i.e., cyclic of order &#039;&#039;f&#039;&#039; if &#039;&#039;q&#039;&#039;=&#039;&#039;p&amp;lt;sup&amp;gt;f&amp;lt;/sup&amp;gt;&#039;&#039; where &#039;&#039;p&#039;&#039; is prime).  The outer automorphism group of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;) is the product of the diagonal automorphism group &#039;&#039;&#039;Z&#039;&#039;&#039;/gcd(3,&#039;&#039;q&#039;&#039;+1)&#039;&#039;&#039;Z&#039;&#039;&#039; (given by the action of &amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;E&amp;lt;sub&amp;gt;6,ad&amp;lt;/sub&amp;gt;(&#039;&#039;q&#039;&#039;)) and the group of field automorphisms (i.e., cyclic of order &#039;&#039;f&#039;&#039; if &#039;&#039;q&#039;&#039;=&#039;&#039;p&#039;&#039;&amp;lt;sup&amp;gt;&#039;&#039;f&#039;&#039;&amp;lt;/sup&amp;gt; where &#039;&#039;p&#039;&#039; is prime).&lt;br /&gt;
&lt;br /&gt;
==Importance in physics==&lt;br /&gt;
&lt;br /&gt;
[[File:E6GUT.svg|300px|right|thumb|The pattern of [[weak isospin]], W, weaker isospin, W&#039;, strong g3 and g8, and baryon minus lepton, B, charges for particles in the [[SO(10)]] [[Grand Unified Theory]], rotated to show the embedding in E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;.]]&lt;br /&gt;
&lt;br /&gt;
N=8 [[supergravity]] in five dimensions, which is a [[dimensional reduction]] from 11 dimensional supergravity, admits an E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; bosonic global symmetry and an Sp(8) bosonic [[gauge symmetry|local symmetry]]. The fermions are in representations of Sp(8), the gauge fields are in a representation of E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;, and the scalars are in a representation of both (Gravitons are [[singlet]]s with respect to both). Physical states are in representations of the coset E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;/Sp(8).&lt;br /&gt;
&lt;br /&gt;
In [[Grand unification theory|grand unification theories]], E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt; appears as a possible gauge group which, after its [[symmetry breaking|breaking]], gives rise to the SU(3) × SU(2) × U(1) [[gauge group]] of the [[standard model]] (also see [[E8 (mathematics)#Importance in physics|Importance in physics of E8]]). One way of achieving this is through breaking to SO(10) × U(1). The adjoint 78 representation breaks, as explained above, into an adjoint 45, spinor 16 and &amp;lt;math&amp;gt;\bar{16}&amp;lt;/math&amp;gt; as well as a singlet of the SO(10) subalgebra. Including the U(1) charge we have&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;78 \rightarrow 45_0 \oplus 16_{-3} \oplus \bar{16}_3 + 1_0. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Where the subscript denotes the U(1) charge.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[En (Lie algebra)]]&lt;br /&gt;
*[[ADE classification]]&lt;br /&gt;
*[[Freudenthal magic square]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*{{Citation | last1=Adams | first1=J. Frank | title=Lectures on exceptional Lie groups | url=http://books.google.com/books?isbn=0226005275 | publisher=[[University of Chicago Press]] | series=Chicago Lectures in Mathematics | isbn=978-0-226-00526-3 | mr=1428422 | year=1996}}&lt;br /&gt;
* {{cite journal|last=Baez|first=John|authorlink=John Baez|year=2002|title=The Octonions, Section 4.4: E&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;|url=http://www.ams.org/bull/2002-39-02/S0273-0979-01-00934-X/home.html|journal=Bull. Amer. Math. Soc.|issn=0273-0979|volume=39|issue=2|pages=145–205|doi=10.1090/S0273-0979-01-00934-X}}. Online HTML version at [http://math.ucr.edu/home/baez/octonions/node17.html].&lt;br /&gt;
* {{cite journal|last=Cremmer|first=E.|coauthors=J. Scherk and J. H. Schwarz|year=1979|title=Spontaneously Broken N=8 Supergravity|url=|journal=Phys. Lett. B|volume=84|issue=1|pages=83–86|doi=10.1016/0370-2693(79)90654-3}}. Online scanned version at [http://ccdb4fs.kek.jp/cgi-bin/img_index?7904075].&lt;br /&gt;
*{{Citation | last1=Dickson | first1=Leonard Eugene | author1-link=Leonard Eugene Dickson | title=A class of groups in an arbitrary realm connected with the configuration of the 27 lines on a cubic surface | url=http://books.google.com/books?id=I_SWAAAAMAAJ&amp;amp;pg=PA145 | id=Reprinted in volume 5 of his collected works | year=1901 | journal=The quarterly journal of pure and applied mathematics | volume=33 | pages=145–173}}&lt;br /&gt;
*{{Citation | last1=Dickson | first1=Leonard Eugene | author1-link=Leonard Eugene Dickson | title=A class of groups in an arbitrary realm connected with the configuration of the 27 lines on a cubic surface (second paper) | url=http://books.google.com/books?id=16J7bgQU65oC&amp;amp;pg=PA145 | id=Reprinted in volume VI of his collected works | year=1908 | journal=The quarterly journal of pure and applied mathematics | volume=39 | pages=205–209}}&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
&lt;br /&gt;
{{Exceptional_Lie_groups}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:E6 (Mathematics)}}&lt;br /&gt;
[[Category:Algebraic groups]]&lt;br /&gt;
[[Category:Lie groups]]&lt;/div&gt;</summary>
		<author><name>131.111.16.20</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Rectangular_potential_barrier&amp;diff=14628</id>
		<title>Rectangular potential barrier</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Rectangular_potential_barrier&amp;diff=14628"/>
		<updated>2013-11-24T21:37:58Z</updated>

		<summary type="html">&lt;p&gt;131.111.184.112: /* E = V0 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Use dmy dates|date=September 2013}}&lt;br /&gt;
{{Use Australian English|date=September 2013}}&lt;br /&gt;
{{infobox television |&lt;br /&gt;
  | image = [[File:Midnightzoo.png|225px|The &#039;&#039;Midnight Zoo&#039;&#039; logo is featured heavily during the show&#039;s broadcast]]&lt;br /&gt;
  | show_name = Midnight Zoo&lt;br /&gt;
  | caption = &#039;&#039;&#039;Midnight Zoo&#039;&#039;&#039;&lt;br /&gt;
  | format = [[Live television|Live]], [[Phone-in]] [[Quiz]] show&lt;br /&gt;
  | runtime = 90 minutes&lt;br /&gt;
  | creator = Ambience Entertainment / Opera Telecom / Telecoms TV&lt;br /&gt;
  | starring  = Angie Richards&amp;lt;br/&amp;gt;Charlotte Connell&amp;lt;br/&amp;gt;[[Steven O&#039;Donnell (Australian actor)|Steven O&#039;Donnell]]&lt;br /&gt;
  | country = [[Australia]]&lt;br /&gt;
  | network = [[Seven Network]]&lt;br /&gt;
  | first_aired = 31 July 2006&lt;br /&gt;
  | last_aired = 21 October 2006&lt;br /&gt;
  | num_episodes = &lt;br /&gt;
  | producer = Jack Dita&lt;br /&gt;
|}}&lt;br /&gt;
&#039;&#039;&#039;&#039;&#039;Midnight Zoo&#039;&#039;&#039;&#039;&#039; was an Australian late-night interactive game show broadcast in parts of [[Australia]] on the [[Seven Network]].  &#039;&#039;Midnight Zoo&#039;&#039; debuted on 31 July 2006 and was broadcast from Sydney. It was shown live throughout [[Victoria (Australia)|Victoria]] and in the capital cities of [[Sydney]] and [[Brisbane]], and ran from 12:30 am to 2:00 am Weekday mornings. The final airing of the show was on 21 October 2006. The show was hosted by [[Steven O&#039;Donnell (Australian actor)|Steven O&#039;Donnell]], Angie Richards, and Charlotte Connell.&lt;br /&gt;
&lt;br /&gt;
== Etymology ==&lt;br /&gt;
The somewhat unusual name of the show stems from the name of the show&#039;s creator, Jack Dita aka &#039;The Zoo Keeper&#039;. The presence of &#039;Midnight&#039; in the name also hints at the show&#039;s late timeslot.&lt;br /&gt;
&lt;br /&gt;
== Cast ==&lt;br /&gt;
Midnight Zoo was hosted by:&amp;lt;br /&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Angie Richards&#039;&#039;&#039; - Host, Hollywood Set&amp;lt;br /&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Charlotte Connell&#039;&#039;&#039; - Host, Bikini Beach Cabana Set&amp;lt;br /&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;[[Steven O&#039;Donnell (Australian actor)|Steven O’Donnell]]&#039;&#039;&#039; - Host, Cash Corner Set&amp;lt;br /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Each host was allocated a location, as shown above.&lt;br /&gt;
&lt;br /&gt;
== Format ==&lt;br /&gt;
Midnight Zoo was similar in concept to the [[Ten Network]]&#039;s ([[Australia]]) &#039;[[The Uplate Game Show|Up Late Game Show]]&#039;, hosted by former [[Big Brother (Australia)|Big Brother]] housemate, Simon Deering aka [[Simon &amp;quot;Hotdogs&amp;quot; Deering|Hotdogs]].&lt;br /&gt;
&lt;br /&gt;
The 90 minute runtime of Midnight Zoo was split into three 30 minute slots. Each slot was allocated to one host/location pair. The puzzles were mostly [[Brainteasers]] and questions relating to popular culture and are regarded as relatively simple (for example, &#039;Name a movie starting with B&#039;). Money is awarded via the gameboard, which dictates the amount of money won for a particular answer. A puzzle featured in a previous slot was carried over to the next slot, suggesting that one puzzle can sometimes occupy the entire 90 minute runtime.&lt;br /&gt;
&lt;br /&gt;
To maintain interest in the show over the course of its duration, there were several segments featured during each slot. These were mostly to encourage callers during slow periods, which in turn encourages human interaction with the show. These include:&amp;lt;br /&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Cash Grab&#039;&#039;&#039; - A 5 minute period where all money on the game board is doubled.&amp;lt;br /&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Double Money&#039;&#039;&#039; - If successful, the next 2 callers will be awarded double their winnings.&amp;lt;br /&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Call Rush&#039;&#039;&#039; - A &amp;quot;short amount of time&amp;quot; where callers are further encouraged to call by on-screen graphics.&lt;br /&gt;
&lt;br /&gt;
All segments came with the added incentive of being featured on live television as a caller. At the same time, a puzzle&#039;s jackpot amount steadily increased throughout the show.&lt;br /&gt;
&lt;br /&gt;
As an added bonus, all successful callers were offered a chance at the Bonus Board. The Bonus Board featured 12 numbers, of which the contestant much choose 3. If the contestant chose all three correctly, their winnings were increased by a jackpot amount which varies from $2500-$12000&lt;br /&gt;
&lt;br /&gt;
==Criticism and problems==&lt;br /&gt;
On 11 August 2006 satirical comedy series &#039;&#039;[[The Chaser&#039;s War on Everything]]&#039;&#039; featured a segment on the influx of late night phone-in quiz shows. The segment mocked the standard of all late night quiz programs and their questions. For &#039;&#039;Midnight Zoo&#039;&#039;, particular reference was made to the female hosts wearing bikinis . &lt;br /&gt;
&lt;br /&gt;
One Australian TV critic has even classed &#039;&#039;Midnight Zoo&#039;&#039; as the worst of the genre [http://www.smh.com.au/news/tv-reviews/midnight-zoo/2006/08/21/1156012463458.html] based on the use of bikinis. &lt;br /&gt;
&lt;br /&gt;
[[Seven Network|Channel Seven&#039;s]] morning program &#039;&#039;[[Sunrise (TV program)|Sunrise]]&#039;&#039; showed a clip one morning of the show the night before where a picture of &#039;&#039;Sunrise&#039;&#039; host [[David Koch (television presenter)|David Koch]] was used in a &amp;quot;name that face&amp;quot; type game. The &#039;&#039;Sunrise&#039;&#039; team criticised the Midnight Zoo for spelling his name wrong and the show in general.&lt;br /&gt;
&lt;br /&gt;
== Probability ==&lt;br /&gt;
The only probability present on Midnight Zoo that can be computed is the chance of success on the Bonus Board. This is equal to &amp;lt;math&amp;gt;12c3&amp;lt;/math&amp;gt; = 1 in 220.&lt;br /&gt;
&lt;br /&gt;
The relative ease of the questions featured on Midnight Zoo suggest easy winnings for contestants. However, one must consider two important factors present in the game that restrict successful callers. Firstly, one must consider the chance of actually being chosen as a contestant. Secondly, one must consider the number of possible answers for the questions with respect to the number of available answers on the game board.&lt;br /&gt;
&lt;br /&gt;
== Pricing and procedure ==&lt;br /&gt;
Midnight Zoo contestants were charged a maximum of 55c/per minute (more from mobiles). The method of player selection was handled by registering interest via SMS or landline. When selected, players would receive a call from Midnight Zoo. Problems arising from this method include Midnight Zoo&#039;s use of a private line, eliminating a number of mobile users who ignore such calls.&lt;br /&gt;
{{Unreferenced|date=January 2007}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Phone-in quiz shows]]&lt;br /&gt;
[[Category:Seven Network shows]]&lt;br /&gt;
[[Category:Australian game shows]]&lt;br /&gt;
[[Category:2000s Australian television series]]&lt;br /&gt;
[[Category:2006 Australian television series debuts]]&lt;br /&gt;
[[Category:2006 Australian television series endings]]&lt;br /&gt;
[[Category:Television shows set in Victoria (Australia)]]&lt;br /&gt;
[[Category:Television shows set in Sydney]]&lt;br /&gt;
[[Category:Television shows set in New South Wales]]&lt;br /&gt;
[[Category:Television shows set in Queensland]]&lt;br /&gt;
[[Category:Television shows set in Australia]]&lt;/div&gt;</summary>
		<author><name>131.111.184.112</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=RC_time_constant&amp;diff=5461</id>
		<title>RC time constant</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=RC_time_constant&amp;diff=5461"/>
		<updated>2013-11-11T20:15:50Z</updated>

		<summary type="html">&lt;p&gt;131.111.219.198: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:Contract-curve-on-edgeworth-box.svg|thumb|400px|right|Blue contract curve showing points of tangency of [[indifference curve]]s in an [[Edgeworth box]]]]&lt;br /&gt;
&lt;br /&gt;
Any [[Walrasian equilibrium]] lies on the contract curve. As with all points that are Pareto efficient, each point on the contract curve is a point of tangency between an indifference curve of one person and an indifference curve of the other person. Thus, on the contract curve the [[marginal rate of substitution]] is the same for both people.&lt;br /&gt;
&lt;br /&gt;
==Example==&lt;br /&gt;
Assume the existence of an economy with two agents, Octavio and Abby, who consume two goods X and Y of which there are fixed supplies, as illustrated in the above Edgeworth box diagram.  Further, assume an initial distribution (endowment) of the goods between Octavio and Abby and let each have normally structured (convex) preferences represented by [[indifference curves]] that are convex toward the people&#039;s respective origins. If the initial allocation is not at a point of tangency between an indifference curve of Octavio and one of Abby, then that initial allocation must be at a point where an indifference curve of Octavio crosses one of Abby. These two indifference curves form a lens shape, with the initial allocation at one of the two corners of the lens. Octavio and Abby will choose to make mutually beneficial trades — that is, they will trade to a point that is on a better (farther from the origin) indifference curve for both. Such a point will be in the interior of the lens, and the rate at which one good will be traded for the other will be between the marginal rate of substitution of Octavio and that of Abby. Since the trades will always provide each person with more of one good and less of the other, trading results in movement upward and to the left, or downward and to the right, in the diagram. &lt;br /&gt;
&lt;br /&gt;
The two people will continue to trade so long as each one’s [[marginal rate of substitution]] (the absolute value of the slope of the person&#039;s indifference curve at that point) differs from that of the other person at the current allocation (in which case there will be a mutually acceptable trading ratio of one good for the other, between the different marginal rates of substitution). At a point where Octavios’s marginal rate of substitution equals Abby’s marginal rate of substitution, no more mutually beneficial exchange is possible.  This point is called a [[Pareto efficient]] equilibrium.  In the Edgeworth box, it is a point at which Octavio’s indifference curve is tangent to Abby’s indifference curve, and it is inside the lens formed by their initial allocations. &lt;br /&gt;
&lt;br /&gt;
Thus the contract curve, the set of points Octavio and Abby could end up at, is the section of the Pareto efficient locus that is in the interior of the lens formed by the initial allocations. The analysis cannot say which particular point along the contract curve they will end up at — this depends on the two people&#039;s bargaining skills.&lt;br /&gt;
&lt;br /&gt;
==Mathematical Explanation==&lt;br /&gt;
In the case of two goods and two individuals, the contract curve can be found as follows. Here &amp;lt;math&amp;gt;x_{2}^{1}&amp;lt;/math&amp;gt; refers to the final amount of good 2 allocated to person 1, etc., &amp;lt;math&amp;gt;u^1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;u^2&amp;lt;/math&amp;gt; refer to the final levels of utility experienced by person 1 and person 2 respectively, &amp;lt;math&amp;gt;u_{0}^{2}&amp;lt;/math&amp;gt; refers to the level of utility that person 2 would receive from the initial allocation without trading at all, and &amp;lt;math&amp;gt;\omega_{1}^{tot}&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\omega_{2}^{tot}&amp;lt;/math&amp;gt; refer to the fixed total quantities available of goods 1 and 2 respectively.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\max_{x_{1}^{1},x_{2}^{1},x_{1}^{2},x_{2}^{2}} u^1(x_{1}^{1},x_{2}^{1})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
subject to:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
x_{1}^{1}+x_{1}^{2} \leq \omega_{1}^{tot}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
x_{2}^{1}+x_{2}^{2} \leq \omega_{2}^{tot}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
u^2(x_{1}^{2},x_{2}^{2}) \geq u_{0}^{2}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This optimization problem states that the goods are to be allocated between the two people in such a way that no more than the available amount of each good is allocated to the two people combined, and the first person&#039;s utility is to be as high as possible while making the second person&#039;s utility no lower than at the initial allocation (so the second person would not refuse to trade from the initial allocation to the point found); this formulation of the problem finds a Pareto efficient point on the  lens, as far as possible from person 1&#039;s origin. This is the point that would be achieved if person 1 had all the bargaining power. (In fact, in order to create at least a slight incentive for person 2 to agree to trade to the identified point, the point would have to be slightly inside the lens.)&lt;br /&gt;
&lt;br /&gt;
In order to trace out the entire contract curve, the above optimization problem can be modified as follows. Maximize a weighted average of the utilities of persons 1 and 2, with weights &#039;&#039;b&#039;&#039; and 1 – &#039;&#039;b&#039;&#039;, subject to the constraints that the allocations of each good not exceed its supply and subject to the constraints that both people&#039;s utilities be at least as great as their utilities at the initial endowments:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\max_{x_{1}^{1},x_{2}^{1},x_{1}^{2},x_{2}^{2}} b \cdot u^1(x_{1}^{1},x_{2}^{1})+ (1-b) \cdot u^2(x_{1}^{2},x_{2}^{2})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
subject to:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
x_{1}^{1}+x_{1}^{2} \leq \omega_{1}^{tot}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
x_{2}^{1}+x_{2}^{2} \leq \omega_{2}^{tot}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
u^1(x_{1}^{1},x_{2}^{1}) \geq u_{0}^{1}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
u^2(x_{1}^{2},x_{2}^{2}) \geq u_{0}^{2}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;u^1&amp;lt;/math&amp;gt; is the utility that person 1 would experience in the absence of trading away from the initial endowment. By varying the weighting parameter &#039;&#039;b&#039;&#039;, one can trace out the entire contract curve: If &#039;&#039;b&#039;&#039; = 1 the problem is the same as the previous problem, and it identifies an efficient point at one edge of the lens formed by the indifference curves of the initial endowment; if &#039;&#039;b&#039;&#039; = 0 all the weight is on person 2&#039;s utility instead of person 1&#039;s, and so the optimization identifies the efficient point on the other edge of the lens. As &#039;&#039;b&#039;&#039; varies smoothly between these two extremes, all the in-between points on the contract curve are traced out.&lt;br /&gt;
&lt;br /&gt;
Note that the above optimizations are not ones that the two people would actually engage in, either explicitly or implicitly. Instead, these optimizations are simply a way for the economist to identify points on the contract curve.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Welfare economics]]&lt;br /&gt;
*[[List of economics topics]].&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*[[Andreu Mas-Colell|Mas-Colell, Andreu]]; Whinston, Michael D.; &amp;amp; Green, Jerry (1995). &#039;&#039;Microeconomic Theory&#039;&#039;. New York: Oxford University Press. ISBN 0-19-510268-1&lt;br /&gt;
&lt;br /&gt;
[[Category:Welfare economics]]&lt;br /&gt;
[[Category:Economics curves]]&lt;/div&gt;</summary>
		<author><name>131.111.219.198</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Rescorla%E2%80%93Wagner_model&amp;diff=7946</id>
		<title>Rescorla–Wagner model</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Rescorla%E2%80%93Wagner_model&amp;diff=7946"/>
		<updated>2013-11-07T10:51:49Z</updated>

		<summary type="html">&lt;p&gt;131.111.185.74: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[financial mathematics]], the &#039;&#039;&#039;Hull–White model&#039;&#039;&#039; is a [[mathematical model|model]] of future [[interest rate]]s. In its most generic formulation, it belongs to the class of no-arbitrage models that are able to fit today&#039;s term structure of interest rates. It is relatively straightforward to translate the mathematical description of the evolution of future interest rates onto a [[Lattice model (finance)|tree or lattice]] and so [[interest rate derivative]]s such as [[bermudan swaption]]s can be valued in the model.&lt;br /&gt;
&lt;br /&gt;
The first Hull–White model was described by [[John C. Hull]] and [[Alan White (economist)|Alan White]] in 1990. The model is still popular in the market today.&lt;br /&gt;
&lt;br /&gt;
==The model==&lt;br /&gt;
&lt;br /&gt;
===One-factor model===&lt;br /&gt;
The model is a [[short-rate model]]. In general, it has dynamics&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;dr(t) = (\theta(t) - \alpha(t) r(t))\,dt + \sigma\, dW(t)\,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
There is a degree of ambiguity amongst practitioners about exactly which parameters in the model are time-dependent or what name to apply to the model in each case.&lt;br /&gt;
The most commonly accepted hierarchy has&lt;br /&gt;
&lt;br /&gt;
:&#039;&#039;θ&#039;&#039; and &#039;&#039;α&#039;&#039; constant – &#039;&#039;&#039;the [[Vasicek model]]&#039;&#039;&#039;&lt;br /&gt;
:&#039;&#039;θ&#039;&#039; has &#039;&#039;t&#039;&#039; dependence – &#039;&#039;&#039;the Hull-White model&#039;&#039;&#039;&lt;br /&gt;
:&#039;&#039;θ&#039;&#039; and &#039;&#039;α&#039;&#039; also time-dependent – &#039;&#039;&#039;the extended [[Vasicek model]]&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
===Two-factor model===&lt;br /&gt;
The two-factor Hull–White model {{harvcol|Hull|2006|pp=657–658}} contains an additional disturbance term whose mean reverts to zero, and is of the form:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;d\,f(r(t)) = \left [\theta(t) + u - \alpha(t)\,f(r(t))\right ]dt + \sigma_1(t)\, dW_1(t)\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\displaystyle u&amp;lt;/math&amp;gt; has an initial value of 0 and follows the process:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;du = -bu\,dt + \sigma_2\,dW_2(t)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Analysis of the one-factor model==&lt;br /&gt;
For the rest of this article we assume only &amp;lt;math&amp;gt;\theta &amp;lt;/math&amp;gt; has t-dependence.&lt;br /&gt;
Neglecting the stochastic term for a moment, notice that the change in r is negative if r is currently &amp;quot;large&amp;quot; (greater than θ(&#039;&#039;t&#039;&#039;)/α) and positive if the current value is small. That is, the stochastic process is a [[mean reversion|mean-reverting]] [[Ornstein–Uhlenbeck process]].&lt;br /&gt;
&lt;br /&gt;
θ is calculated from the initial [[yield curve]] describing the current term structure of interest rates. Typically α is left as a user input (for example it may be estimated from historical data). σ is determined via [[calibration]] to a set of [[caplet]]s and [[swaption]]s readily tradeable in the market.&lt;br /&gt;
&lt;br /&gt;
When &amp;lt;math&amp;gt;\alpha&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\theta&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt; are constant, [[Itô&#039;s lemma]] can be used to prove that&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; r(t) = e^{-\alpha t}r(0) +  \frac{\theta}{\alpha} \left(1- e^{-\alpha t}\right) + \sigma e^{-\alpha t}\int_0^t e^{\alpha u}\,dW(u)\,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
which has distribution&lt;br /&gt;
:&amp;lt;math&amp;gt;r(t) \sim N\left(e^{-\alpha t} r(0) +  \frac{\theta}{\alpha} \left(1- e^{-\alpha t}\right), \frac{\sigma^2}{2\alpha} \left(1-e^{-2\alpha t}\right)\right).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;N( \cdot ,\cdot )&amp;lt;/math&amp;gt; is the [[normal distribution]].&lt;br /&gt;
&lt;br /&gt;
==Bond pricing using the Hull–White model==&lt;br /&gt;
&lt;br /&gt;
It turns out that the time-&#039;&#039;S&#039;&#039; value of the &#039;&#039;T&#039;&#039;-maturity [[discount bond]] has distribution (note the &#039;&#039;affine term&#039;&#039; structure here!)&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;P(S,T) = A(S,T)\exp(-B(S,T)r(S))\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; B(S,T) = \frac{1-\exp(-\alpha(T-S))}{\alpha} \,&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; A(S,T) = \frac{P(0,T)}{P(0,S)}\exp\left( \,  -B(S,T) \frac{\partial\log(P(0,S))}{\partial S} - \frac{\sigma^2(\exp(-\alpha T)-\exp(-\alpha S))^2(\exp(2\alpha S)-1)}{4\alpha^3}\right) \,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Note that their terminal distribution for &#039;&#039;P&#039;&#039;(&#039;&#039;S&#039;&#039;,&#039;&#039;T&#039;&#039;) is [[log-normal distribution|distributed log-normally]].&lt;br /&gt;
&lt;br /&gt;
==Derivative pricing==&lt;br /&gt;
&lt;br /&gt;
By selecting as [[numeraire]] the time-&#039;&#039;S&#039;&#039; bond (which corresponds to switching to the S-forward measure), we have from the [[fundamental theorem of arbitrage-free pricing]], the value at time 0 of a derivative which has payoff at time &#039;&#039;S&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;V(t) = P(t,S)\mathbb{E}_S[V(S)| \mathcal{F}(t)].\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Here, &amp;lt;math&amp;gt;\mathbb{E}_S&amp;lt;/math&amp;gt; is the expectation taken with respect to the [[forward measure]]. Moreover that standard arbitrage arguments show&lt;br /&gt;
that the time &#039;&#039;T&#039;&#039; forward price &amp;lt;math&amp;gt;F_V(t,T)&amp;lt;/math&amp;gt; for a payoff at time &#039;&#039;T&#039;&#039; given by &#039;&#039;V(T)&#039;&#039; must satisfy &amp;lt;math&amp;gt;F_V(t,T) = V(t)/P(t,S)&amp;lt;/math&amp;gt;, thus&lt;br /&gt;
:&amp;lt;math&amp;gt;F_V(t,T) = \mathbb{E}_T[V(T)|\mathcal{F}(t)].\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus it is possible to value many derivatives &#039;&#039;V&#039;&#039; dependent solely on a single bond &#039;&#039;P&#039;&#039;(&#039;&#039;S&#039;&#039;,&#039;&#039;T&#039;&#039;) analytically when working in the Hull–White model. For example in the case of a [[put option|bond put]]&lt;br /&gt;
:&amp;lt;math&amp;gt;V(S) = (K-P(S,T))^+.\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Because &#039;&#039;P&#039;&#039;(&#039;&#039;S&#039;&#039;,&#039;&#039;T&#039;&#039;) is lognormally distributed, the general calculation&lt;br /&gt;
used for Black-Scholes shows that&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;{E}_S[(K-P(S,T))^{+}] = KN(-d_2) - F(t,S,T)N(d_1)\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;d_1 = \frac{\log(F/K) + \sigma_P^2S/2}{\sigma_P \sqrt{S}}\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;d_2 = d_1 - \sigma_P \sqrt{S}.\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Thus today&#039;s value (with the &#039;&#039;P&#039;&#039;(0,&#039;&#039;S&#039;&#039;) multiplied back in) is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;P(0,S)KN(-d_2) - P(0,T)N(-d_1)\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Here σ&amp;lt;sub&amp;gt;&#039;&#039;P&#039;&#039;&amp;lt;/sub&amp;gt; is the standard deviation of the&lt;br /&gt;
log-normal distribution for &#039;&#039;P&#039;&#039;(&#039;&#039;S&#039;&#039;,&#039;&#039;T&#039;&#039;). A fairly substantial amount&lt;br /&gt;
of algebra shows that it is related to the original parameters via&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sqrt{S}\sigma_P&lt;br /&gt;
=\frac{\sigma}{\alpha}(1-\exp(-\alpha(T-S)))\sqrt{\frac{1-\exp(-2\alpha S)}{2\alpha}}\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Note that this expectation was done in the S-bond measure, whereas we did not specify a measure at all for the original Hull-White process. This does not matter — the volatility is all that matters and is measure-independent.&lt;br /&gt;
&lt;br /&gt;
Because [[interest rate caps/floors]] are equivalent to bond puts and calls respectively, the above analysis shows that caps and floors can be priced analytically in the Hull–White model. [[Jamshidian&#039;s trick]] applies to Hull-White (as today&#039;s value of a swaption in HW is a [[monotonic function]] of today&#039;s short rate). Thus knowing how to price caps is also sufficient for pricing swaptions. &lt;br /&gt;
&lt;br /&gt;
The swaptions can also be priced directly as described in Henrard (2003). The direct implementation is usually more efficient.&lt;br /&gt;
&lt;br /&gt;
==Trees and lattices==&lt;br /&gt;
However, valuing vanilla instruments such as caps and swaptions is useful primarily for calibration. The real use of the model is to value somewhat more [[exotic derivatives]] such as [[bermudan swaption]]s on a [[Lattice model (finance)|lattice]], or other derivatives in a multi-currency context such as Quanto Constant Maturity Swaps, as explained for example in Brigo and Mercurio (2001).&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Vasicek model]]&lt;br /&gt;
*[[Cox–Ingersoll–Ross model]]&lt;br /&gt;
*[[Black-Karasinski model]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Primary references&#039;&#039;&#039;&lt;br /&gt;
*John Hull and Alan White, &amp;quot;Using Hull-White interest rate trees,&amp;quot; Journal of Derivatives, Vol. 3, No. 3 (Spring 1996), pp 26–36&lt;br /&gt;
*John Hull and Alan White, &amp;quot;Numerical procedures for implementing term structure models I,&amp;quot; Journal of Derivatives, Fall 1994, pp 7–16&lt;br /&gt;
*John Hull and Alan White, &amp;quot;Numerical procedures for implementing term structure models II,&amp;quot; Journal of Derivatives, Winter 1994, pp 37–48&lt;br /&gt;
*John Hull and Alan White, &amp;quot;The pricing of options on interest rate caps and floors using the Hull–White model&amp;quot; in Advanced Strategies in Financial Risk Management, Chapter 4, pp 59–67.&lt;br /&gt;
*John Hull and Alan White, &amp;quot;One factor interest rate models and the valuation of interest rate derivative securities,&amp;quot; Journal of Financial and Quantitative Analysis, Vol 28, No 2, (June 1993) pp 235–254&lt;br /&gt;
*John Hull and Alan White, &amp;quot;Pricing interest-rate derivative securities&amp;quot;, The Review of Financial Studies, Vol 3, No. 4 (1990) pp.&amp;amp;nbsp;573–592&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Other references&#039;&#039;&#039;&lt;br /&gt;
*{{cite book |last= Hull|first= John C.|authorlink= John C. Hull|title= Options, Futures, and Other Derivatives|edition= 6th|year=2006 |publisher= [[Prentice Hall]] |location= [[Upper Saddle River, New Jersey|Upper Saddle River, N.J]] |isbn= 0-13-149908-4 |oclc= 60321487 |pages= 657–658 |chapter= Interest Rate Derivatives: Models of the Short Rate |ref=harv |lccn= 2005047692 }}&lt;br /&gt;
*{{cite book | title = Interest Rate Models&amp;amp;nbsp;— Theory and Practice with Smile, Inflation and Credit| author = [[Damiano Brigo]], [[Fabio Mercurio]] | publisher = Springer Verlag | year = 2001 | edition = 2nd ed. 2006 | isbn = 978-3-540-22149-4}}&lt;br /&gt;
*Henrard, Marc (2003). Explicit Bond Option and Swaption Formula in Heath-Jarrow-Morton One Factor Model, &#039;&#039;International Journal of Theoretical and Applied Finance&#039;&#039;, 6(1), 57-72. [http://ssrn.com/abstract=434860 Preprint SSRN].&lt;br /&gt;
*Henrard, Marc (2009). Efficient swaptions price in Hull-White one factor model, arXiv, 0901.1776v1. [http://arxiv.org/abs/0901.1776 Preprint arXiv].&lt;br /&gt;
*Eugen Puschkarski, [http://web.archive.org/web/*/www.angelfire.com/ny/financeinfo/Diplomnew.ppt &#039;&#039;Implementation of Hull-White´s No-Arbitrage Term Structure Model&#039;&#039;], Diploma Thesis, Center for Central European Financial Markets&lt;br /&gt;
*Letian Wang, [http://letianwang.net/Fixed_Income/09_Hull-White_Model.htm &#039;&#039;Hull-White Model&#039;&#039;], Fixed Income Quant Group, DTCC (detailed numeric example and derivation)&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Online utilities&#039;&#039;&#039;&lt;br /&gt;
*[http://lombok.demon.co.uk/financialTap/interestrates/hwtrinomialtree Hull-White Trinomial Tree], Dr. S.H. Man, Turaz.&lt;br /&gt;
*[http://lombok.demon.co.uk/financialTap/montecarlo/hullwhite Short Rates Simulation using Hull White Model], Dr. S.H. Man, Turaz.&lt;br /&gt;
&lt;br /&gt;
{{Bond market}}&lt;br /&gt;
{{Stochastic processes}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Hull-White model}}&lt;br /&gt;
[[Category:Finance theories]]&lt;br /&gt;
[[Category:Mathematical finance]]&lt;br /&gt;
[[Category:Interest rates]]&lt;br /&gt;
[[Category:Fixed income analysis]]&lt;br /&gt;
[[Category:Short-rate models]]&lt;/div&gt;</summary>
		<author><name>131.111.185.74</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Half_range_Fourier_series&amp;diff=11545</id>
		<title>Half range Fourier series</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Half_range_Fourier_series&amp;diff=11545"/>
		<updated>2013-11-04T02:05:46Z</updated>

		<summary type="html">&lt;p&gt;131.111.184.92: lowered k index by including it in the subscript&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[probability theory]] and [[statistical mechanics]], a &#039;&#039;&#039;Gibbs state&#039;&#039;&#039; is an equilibrium probability distribution which remains invariant under future evolution of the system.  For example, a stationary or steady-state distribution of a [[Markov chain]], such as that achieved by running a [[Markov chain Monte Carlo]] iteration for a sufficiently long time, is a Gibbs state.&lt;br /&gt;
&lt;br /&gt;
Precisely, suppose &amp;lt;math&amp;gt;L \;&amp;lt;/math&amp;gt; is a generator of evolutions for an initial state &amp;lt;math&amp;gt;\rho_0 \;&amp;lt;/math&amp;gt;, so that the state at any later time is given by &amp;lt;math&amp;gt;\rho(t) = e^{L t} [\rho_0] \;&amp;lt;/math&amp;gt;.  Then the condition for &amp;lt;math&amp;gt;\rho_{\infty} \;&amp;lt;/math&amp;gt; to be a Gibbs state is&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;L [\rho_{\infty}] = 0 &amp;lt;/math&amp;gt; .&lt;br /&gt;
&lt;br /&gt;
In [[physics]] there may be several physically distinct Gibbs states in which a system may be trapped, particularly at lower temperatures. &lt;br /&gt;
&lt;br /&gt;
They are named after [[Josiah Willard Gibbs]], for his work in determining equilibrium properties of [[statistical ensemble]]s. Gibbs himself referred to this type of statistical ensemble as being in &amp;quot;statistical equilibrium&amp;quot;.&amp;lt;ref name=&amp;quot;gibbs&amp;quot;&amp;gt;{{cite book |last=Gibbs |first=Josiah Willard |authorlink=Josiah Willard Gibbs |title=[[Elementary Principles in Statistical Mechanics|Elementary Principles in Statistical Mechanics, developed with especial reference to the rational foundation of thermodynamics]] |year=1902 |publisher=[[Charles Scribner&#039;s Sons]] |location=New York}}&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Gibbs algorithm]]&lt;br /&gt;
* [[Gibbs measure]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
&lt;br /&gt;
{{mathapplied-stub}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Statistical mechanics]]&lt;br /&gt;
[[Category:Probability theory]]&lt;br /&gt;
[[Category:Stochastic processes]]&lt;/div&gt;</summary>
		<author><name>131.111.184.92</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Taub%E2%80%93NUT_space&amp;diff=21782</id>
		<title>Taub–NUT space</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Taub%E2%80%93NUT_space&amp;diff=21782"/>
		<updated>2013-10-28T11:01:07Z</updated>

		<summary type="html">&lt;p&gt;131.111.16.20: It&amp;#039;s not homogeneous.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Hilbert C*-modules&#039;&#039;&#039; are [[mathematical object]]s which generalise the notion of a [[Hilbert space]] (which itself is a generalisation of [[Euclidean space]]), in that they endow a [[vector space|linear space]] with an &amp;quot;[[inner product]]&amp;quot; which takes values in a [[C*-algebra]].  Hilbert C*-modules were first introduced in the work of [[Irving Kaplansky]] in [[1953 in science|1953]], which developed the theory for [[commutative]], [[unital algebra]]s (though Kaplansky observed that the assumption of a unit element was not &amp;quot;vital&amp;quot;).&amp;lt;ref&amp;gt;{{cite journal| last = Kaplansky| first = I.| authorlink = Irving Kaplansky| title = Modules over operator algebras| journal = [[American Journal of Mathematics]]| volume = 75| issue = 4| pages = 839–853| year = 1953| doi = 10.2307/2372552| jstor = 2372552}}&amp;lt;/ref&amp;gt; In the 1970s the theory was extended to non-commutative C*-algebras independently by William Lindall Paschke&amp;lt;ref&amp;gt;{{cite journal| last = Paschke| first = W. L.| title = Inner product modules over B*-algebras| journal = [[Transactions of the American Mathematical Society]]| volume = 182| pages = 443–468| year = 1973| doi = 10.2307/1996542| jstor = 1996542}}&amp;lt;/ref&amp;gt; and Marc Aristide Rieffel, the latter in a paper which used Hilbert C*-modules to construct a theory of [[induced representation]]s of C*-algebras.&amp;lt;ref&amp;gt;{{cite journal| last = Rieffel| first = M. A.| title = Induced representations of C*-algebras| journal = Advances in Mathematics| volume = 13| pages = 176–257| publisher = [[Elsevier]]| year = 1974| doi = 10.1016/0001-8708(74)90068-1| issue = 2}}&amp;lt;/ref&amp;gt; Hilbert C*-modules are crucial to Kasparov&#039;s formulation of [[KK-theory]],&amp;lt;ref&amp;gt;{{cite journal| last = Kasparov| first = G. G.| title = Hilbert C*-modules: Theorems of Stinespring and Voiculescu| journal = Journal of Operator Theory| volume = 4| pages = 133–150| publisher = Theta Foundation| year = 1980}}&amp;lt;/ref&amp;gt; and provide the right framework to extend the notion of [[Morita equivalence]] to [[C*-algebras]].&amp;lt;ref&amp;gt;{{cite journal| last = Rieffel| first = M. A.| title = Morita equivalence for operator algebras| journal = Proceedings of Symposia in Pure Mathematics| volume = 38| pages = 176–257| publisher = American Mathematical Society| year = 1982}}&amp;lt;/ref&amp;gt; They can be viewed as the generalization of [[vector bundles]] to noncommutative [[C*-algebras]] and as such play an important role in [[noncommutative geometry]], notably in [[C*-algebraic quantum group theory]],&amp;lt;ref&amp;gt;{{cite journal| last = Baaj| first = S.| coauthors = Skandalis, G.| title = Unitaires multiplicatifs et dualité pour les produits croisés de C*-algèbres| journal = [[Annales Scientifiques de l&#039;École Normale Supérieure]]| volume = 26| issue = 4| pages = 425–488| year = 1993}}&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;{{cite journal| last = Woronowicz| first = S. L.| authorlink = S. L. Woronowicz| title = Unbounded elements affiliated with C*-algebras and non-compact quantum groups| journal = Communications in Mathematical Physics| volume = 136| pages = 399–432| year = 1991| doi = 10.1007/BF02100032|bibcode = 1991CMaPh.136..399W| issue = 2 }}&amp;lt;/ref&amp;gt; and [[groupoid]] [[C*-algebras]].&lt;br /&gt;
&lt;br /&gt;
== Definitions ==&lt;br /&gt;
&lt;br /&gt;
=== Inner-product &#039;&#039;A&#039;&#039;-modules ===&lt;br /&gt;
Let &#039;&#039;A&#039;&#039; be a C*-algebra (not assumed to be commutative or unital), its [[Involution (mathematics)|involution]] denoted by *. An &#039;&#039;&#039;inner-product &#039;&#039;A&#039;&#039;-module&#039;&#039;&#039; (or &#039;&#039;&#039;pre-Hilbert &#039;&#039;A&#039;&#039;-module&#039;&#039;&#039;) is a [[complex number|complex]] linear space &#039;&#039;E&#039;&#039; which is equipped with a compatible right [[Module (mathematics)|&#039;&#039;A&#039;&#039;-module]] structure, together with a map&lt;br /&gt;
:&amp;lt;math&amp;gt; \langle \cdot, \cdot \rangle : E \times E \rightarrow A &amp;lt;/math&amp;gt;&lt;br /&gt;
which satisfies the following properties:&lt;br /&gt;
&lt;br /&gt;
*For all &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039;, &#039;&#039;z&#039;&#039; in &#039;&#039;E&#039;&#039;, and α, β in &#039;&#039;&#039;C&#039;&#039;&#039;:&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt; \langle x, \alpha y + \beta z \rangle = \alpha \langle x, y \rangle + \beta \langle x, z \rangle&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:(&#039;&#039;i.e.&#039;&#039; the inner product is linear in its second argument).&lt;br /&gt;
&lt;br /&gt;
*For all &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039; in &#039;&#039;E&#039;&#039;, and &#039;&#039;a&#039;&#039; in &#039;&#039;A&#039;&#039;:&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt; \langle x, ya \rangle = \langle x, y \rangle a&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
*For all &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039; in &#039;&#039;E&#039;&#039;:&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt; \langle x, y \rangle = \langle y, x \rangle^*,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:from which it follows that the inner product is [[conjugate linear]] in its first argument (&#039;&#039;i.e.&#039;&#039; it is a [[sesquilinear form]]).&lt;br /&gt;
&lt;br /&gt;
*For all &#039;&#039;x&#039;&#039; in &#039;&#039;E&#039;&#039;:&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt; \langle x, x \rangle \geq 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:and&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt; \langle x, x \rangle = 0 \iff x = 0.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:(An element of a C*-algebra &#039;&#039;A&#039;&#039; is said to be &#039;&#039;positive&#039;&#039; if it is [[self-adjoint]] with non-negative [[Spectrum (functional analysis)|spectrum]].)&amp;lt;ref&amp;gt;{{cite book| last = Arveson| first = William| authorlink = William Arveson|title = An Invitation to C*-Algebras| publisher = Springer-Verlag| year = 1976| page = 35}}&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;In the case when &#039;&#039;A&#039;&#039; is non-unital, the spectrum of an element is calculated in the C*-algebra generated by adjoining a unit to &#039;&#039;A&#039;&#039;.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Hilbert &#039;&#039;A&#039;&#039;-modules ===&lt;br /&gt;
An analogue to the [[Cauchy-Schwarz inequality]] holds for an inner-product &#039;&#039;A&#039;&#039;-module &#039;&#039;E&#039;&#039;:&amp;lt;ref&amp;gt;This result in fact holds for semi-inner-product &#039;&#039;A&#039;&#039;-modules, which may have non-zero elements &#039;&#039;x&#039;&#039; such that &amp;lt;&#039;&#039;x&#039;&#039;,&#039;&#039;x&#039;&#039;&amp;gt; = 0, as the proof does not rely on the [[nondegeneracy]] property.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle x, y \rangle \langle y, x \rangle \leq \Vert \langle x, x \rangle \Vert \langle y, y \rangle&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for &#039;&#039;x&#039;&#039;, &#039;&#039;y&#039;&#039; in &#039;&#039;E&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
On the pre-Hilbert module &#039;&#039;E&#039;&#039;, define a norm by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Vert x \Vert = \Vert \langle x, x \rangle \Vert^\frac{1}{2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The norm-completion of &#039;&#039;E&#039;&#039;, still denoted by &#039;&#039;E&#039;&#039;, is said to be a &#039;&#039;&#039;Hilbert &#039;&#039;A&#039;&#039;-module&#039;&#039;&#039; or a &#039;&#039;&#039;Hilbert C*-module over the C*-algebra &#039;&#039;A&#039;&#039;&#039;&#039;&#039;.&lt;br /&gt;
The Cauchy-Schwarz inequality implies the inner product is jointly continuous in norm and can therefore be extended to the completion.&lt;br /&gt;
&lt;br /&gt;
The action of &#039;&#039;A&#039;&#039; on &#039;&#039;E&#039;&#039; is continuous: for all &#039;&#039;x&#039;&#039; in &#039;&#039;E&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;a_{\lambda} \rightarrow a \Rightarrow xa_{\lambda} \rightarrow xa.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Similarly, if {&#039;&#039;e&amp;lt;sub&amp;gt;λ&amp;lt;/sub&amp;gt;&#039;&#039;} is an [[Approximate identity|approximate unit]] for &#039;&#039;A&#039;&#039; (a [[Net (mathematics)|net]] of self-adjoint elements of &#039;&#039;A&#039;&#039; for which &#039;&#039;ae&#039;&#039;&amp;lt;sub&amp;gt;λ&amp;lt;/sub&amp;gt; and &#039;&#039;e&#039;&#039;&amp;lt;sub&amp;gt;λ&amp;lt;/sub&amp;gt;&#039;&#039;a&#039;&#039; tend to &#039;&#039;a&#039;&#039; for each &#039;&#039;a&#039;&#039; in &#039;&#039;A&#039;&#039;), then for &#039;&#039;x&#039;&#039; in &#039;&#039;E&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; xe_\lambda \rightarrow x&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
whence it follows that &#039;&#039;EA&#039;&#039; is [[Dense set|dense]] in &#039;&#039;E&#039;&#039;, and &#039;&#039;x&#039;&#039;1 = &#039;&#039;x&#039;&#039; when &#039;&#039;A&#039;&#039; is unital.&lt;br /&gt;
 &lt;br /&gt;
Let&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \langle E, E \rangle = \operatorname{span} \{ \langle x, y \rangle | x, y \in E \},&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
then the [[Closure (topology)|closure]] of &amp;lt;&#039;&#039;E&#039;&#039;,&#039;&#039;E&#039;&#039;&amp;gt; is a two-sided ideal in &#039;&#039;A&#039;&#039;. Two-sided ideals are C*-subalgebras and therefore possess approximate units. One can verify that &#039;&#039;E&#039;&#039;&amp;lt;&#039;&#039;E&#039;&#039;,&#039;&#039;E&#039;&#039;&amp;gt; is dense in &#039;&#039;E&#039;&#039;. In the case when &amp;lt;&#039;&#039;E&#039;&#039;,&#039;&#039;E&#039;&#039;&amp;gt; is dense in &#039;&#039;A&#039;&#039;, &#039;&#039;E&#039;&#039; is said to be &#039;&#039;&#039;full&#039;&#039;&#039;. This does not generally hold.&lt;br /&gt;
&lt;br /&gt;
== Examples ==&lt;br /&gt;
&lt;br /&gt;
=== Hilbert spaces ===&lt;br /&gt;
A complex Hilbert space &#039;&#039;H&#039;&#039; is a Hilbert &#039;&#039;&#039;C&#039;&#039;&#039;-module under its inner product, the complex numbers being a C*-algebra with an involution given by [[complex conjugation]].&lt;br /&gt;
&lt;br /&gt;
===Vector bundles===&lt;br /&gt;
If &#039;&#039;X&#039;&#039; is a [[locally compact Hausdorff space]] and &#039;&#039;E&#039;&#039; a [[vector bundle]] over &#039;&#039;X&#039;&#039; with a [[Riemannian metric]] &#039;&#039;g&#039;&#039;, then the space of continuous sections of &#039;&#039;E&#039;&#039; is a Hilbert &#039;&#039;C(X)&#039;&#039;-module. The inner product is given by&lt;br /&gt;
::&amp;lt;math&amp;gt; \langle f,h\rangle (x):=g(f(x),h(x)).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The converse holds as well: Every countably generated Hilbert C*-module over a commutative C*-algebra &#039;&#039;A = C(X)&#039;&#039;  is isomorphic to the space of sections vanishing at infinity of a continuous field of Hilbert spaces over &#039;&#039;X&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
=== C*-algebras ===&lt;br /&gt;
Any C*-algebra &#039;&#039;A&#039;&#039; is a Hilbert &#039;&#039;A&#039;&#039;-module under the inner product &amp;lt;&#039;&#039;a&#039;&#039;,&#039;&#039;b&#039;&#039;&amp;gt; = &#039;&#039;a&#039;&#039;*&#039;&#039;b&#039;&#039;.  By the C*-identity, the Hilbert module norm coincides with C*-norm on &#039;&#039;A&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
The (algebraic) [[direct sum of modules|direct sum]] of &#039;&#039;n&#039;&#039; copies of &#039;&#039;A&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; A^n = \oplus_1^n A&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
can be made into a Hilbert &#039;&#039;A&#039;&#039;-module by defining&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle (a_i), (b_i) \rangle = \sum a_i^* b_i.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One may also consider the following elements in the countable direct product of &#039;&#039;A&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathcal{H}_A = \{ (a_i) | \sum a_i^{*}a_i\text{ converges in }A \}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Given an inner product analogous to that on &#039;&#039;A&amp;lt;sup&amp;gt;n&amp;lt;/sup&amp;gt;&#039;&#039;, the resulting Hilbert &#039;&#039;A&#039;&#039;-module is called the &#039;&#039;&#039;standard Hilbert module&#039;&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Operator algebra]]&lt;br /&gt;
&lt;br /&gt;
== Notes ==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* {{cite book |last=Lance |first=E. Christopher|title=Hilbert C*-modules: A toolkit for operator algebraists |series=London Mathematical Society Lecture Note Series|year=1995 |publisher=Cambridge University Press |location=Cambridge, England}}&lt;br /&gt;
&lt;br /&gt;
== External links ==&lt;br /&gt;
* {{MathWorld |title=Hilbert C*-Module |urlname=HilbertC-Star-Module}}&lt;br /&gt;
* [http://www.imn.htwk-leipzig.de/~mfrank/hilmod.html Hilbert C*-Modules Home Page], a literature list&lt;br /&gt;
&lt;br /&gt;
[[Category:C*-algebras]]&lt;br /&gt;
[[Category:Operator theory]]&lt;br /&gt;
[[Category:Theoretical physics]]&lt;/div&gt;</summary>
		<author><name>131.111.16.20</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Ward%E2%80%93Takahashi_identity&amp;diff=26384</id>
		<title>Ward–Takahashi identity</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Ward%E2%80%93Takahashi_identity&amp;diff=26384"/>
		<updated>2013-10-19T19:40:10Z</updated>

		<summary type="html">&lt;p&gt;131.111.204.168: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Condensed matter physics}}&lt;br /&gt;
&#039;&#039;&#039;Surface plasmon polaritons&#039;&#039;&#039; (SPPs), are [[infrared]] or [[visible spectrum|visible]]-frequency [[electromagnetic waves]], which travel along a [[metal]]-[[dielectric]] or metal-air interface. The term &amp;quot;surface plasmon polariton&amp;quot; explains that the wave involves both charge motion in the metal (&amp;quot;[[surface plasmon]]&amp;quot;) and electromagnetic waves in the air or dielectric (&amp;quot;[[polariton]]&amp;quot;)&lt;br /&gt;
&lt;br /&gt;
They are a type of [[surface wave]], guided along the interface in much the same way that light can be guided by an optical fiber. SPPs are shorter in wavelength than the incident light (photons).&amp;lt;ref name=nist-plasmo-mm/&amp;gt; Hence, SPPs can have tighter [[laser|spatial confinement]] and higher [[field intensity|local field intensity]].&amp;lt;ref name=nist-plasmo-mm/&amp;gt; Perpendicular to the interface, they have subwavelength-scale confinement. An SPP will propagate along the interface until its energy is lost either to either absorption in the metal or scattering into other directions (such as into free space).&lt;br /&gt;
&lt;br /&gt;
Application of SPPs enables [[subwavelength optics]] in microscopy and [[lithography]] beyond the [[diffraction limit]]. It also enables the first steady-state micro-mechanical measurement of a fundamental property of light itself: the momentum of a photon in a dielectric medium. Other applications are [[photonic]] data storage, light generation, and bio-photonics.&amp;lt;ref name=nist-plasmo-mm&amp;gt;&lt;br /&gt;
{{cite web&lt;br /&gt;
  | last =NIST researchers &lt;br /&gt;
  | first =Nanofabrication Research Group  &lt;br /&gt;
  | title =Three-Dimensional Plasmonic Metamaterials &lt;br /&gt;
  | publisher =National Institute of Science and Technology &lt;br /&gt;
  | date = &lt;br /&gt;
  | url =http://www.nist.gov/cnst/nrg/3d_plasmonic_metamaterials.cfm &lt;br /&gt;
  | accessdate =2011-02-15}}&lt;br /&gt;
*{{cite web&lt;br /&gt;
  | last =NIST researchers &lt;br /&gt;
  | first =Nanofabrication Research Group  &lt;br /&gt;
  | title =Opto-mechanical Devices for Measuring Nanoplasmonic Metamaterials &lt;br /&gt;
  | publisher =National Institute of Science and Technology &lt;br /&gt;
  | date = &lt;br /&gt;
  | url =http://www.nist.gov/cnst/nrg/nanoplasmonic_lab.cfm&lt;br /&gt;
  | accessdate =2011-02-15}}&lt;br /&gt;
*{{NIST-PD|article=Three-Dimensional Plasmonic  Metamaterials |url=http://www.nist.gov/cnst/nrg/3d_plasmonic_metamaterials.cfm}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=berkely-grin&amp;gt;&lt;br /&gt;
{{cite web&lt;br /&gt;
  | last =Yarris  &lt;br /&gt;
  | first =Lynn  &lt;br /&gt;
  | title =GRIN Plasmonics... &lt;br /&gt;
  | publisher =U.S. Department of Energy National Laboratory Operated by the University of California &lt;br /&gt;
  | date = &lt;br /&gt;
  | url =http://www.nist.gov/cnst/nrg/3d_plasmonic_metamaterials.cfm &lt;br /&gt;
  | format =Online news release &lt;br /&gt;
  | accessdate =2011-02-15}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=w-barnes&amp;gt;&lt;br /&gt;
{{cite journal&lt;br /&gt;
|last1=Barnes|first1=William L.|last2=Dereux|first2=Alain|last3=Ebbesen|first3=Thomas W.|title=Surface plasmon subwavelength optics|doi=10.1038/nature01937|pmid=12917696|year=2003|page=824|issue=6950|volume=424&lt;br /&gt;
|journal=Nature&lt;br /&gt;
|url=http://www.nature.com/nature/journal/v424/n6950/pdf/nature01937.pdf&lt;br /&gt;
|bibcode = 2003Natur.424..824B }} &lt;br /&gt;
*{{cite journal |last1=Huidobro |first1=Paloma A. |last2=Nesterov |first2=Maxim L. |last3=Martín-Moreno |first3=Luis |last4=García-Vidal |first4=Francisco J. |doi=10.1021/nl100800c |title=Transformation Optics for Plasmonics |pmid=20465271 |year=2010 |page=1985 |issue=6 |volume=10 |journal=Nano Letters|url=http://www.uam.es/gruposinv/nanophot/Web_grupo_archivos/papers/huidobro_june2010.pdf|bibcode = 2010NanoL..10.1985H |arxiv = 1003.1154 }} Free PDF download for these peer reviewed articles.&lt;br /&gt;
*PDF from arxiv.org - [http://arxiv.org/PS_cache/arxiv/pdf/1003/1003.1154v2.pdf Transformation Optics for Plasmonics]. 15 pages.&amp;lt;/ref&amp;gt;&amp;lt;ref name=nanoplasmonics/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Excitation==&lt;br /&gt;
&lt;br /&gt;
{{Multiple image|direction=vertical|align=right|image1=Prism_Coupler.png|image2=Grating_Coupler.png|width=300|caption1=Figure 1: (a) Kretschmann and (b) Otto configuration of an Attenuated Total Reflection setup for coupling surface plasmons. In both cases, the surface plasmon propagates along the metal/dielectric interface {{anchor|fig2anchor}}|caption2=Figure 2: Grating Coupler for Surface Plasmons. The wave vector is increased by the spatial frequency }}&lt;br /&gt;
SPPs can be excited by both electrons and photons. Excitation by electrons is created by firing electrons into the bulk of a metal. As the electrons scatter, energy is transferred into the bulk plasma. The component of the scattering vector parallel to the surface results in the formation of a surface plasmon polariton.&amp;lt;ref&amp;gt;{{cite journal|author=S.Zeng &#039;&#039;et al.&#039;&#039;|title=Size dependence of Au NP-enhanced surface plasmon resonance based on differential phase measurement |journal=Sensors and Actuators B: Chemical |year=2012|doi=10.1016/j.snb.2012.09.073|last2=Yu|first2=Xia|last3=Law|first3=Wing-Cheung|last4=Zhang|first4=Yating|last5=Hu|first5=Rui|last6=Dinh|first6=Xuan-Quyen|last7=Ho|first7=Ho-Pui|last8=Yong|first8=Ken-Tye|volume=176|pages=1128 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If a free-space photon comes from air towards a smooth metal surface, it &#039;&#039;cannot&#039;&#039; excite an SPP at the metal-air interface. The reason is that if the photon and SPP have the same frequency, then they necessarily have different in-plane wavevectors. This incompatibility is analogous to the lack of transmission that occurs during [[total internal reflection]]. Analogously, an SPP on a smooth metal surface &#039;&#039;cannot&#039;&#039; lose energy to radiation into the dielectric (if the dielectric is uniform).&lt;br /&gt;
&lt;br /&gt;
Nevertheless, coupling of photons into SPPs can be achieved using a coupling medium such as a [[Prism (optics)|prism]] or grating to match the photon and surface plasmon wave vectors. A prism can be positioned against a thin metal film in the Kretschmann configuration or very close to a metal surface in the Otto configuration (Figure 1). A grating coupler matches the wave vectors by increasing the parallel wave vector component by an amount related to the grating period (Figure 2). This method, while less frequently utilized, is critical to the theoretical understanding of the effect of surface [[surface roughness|roughness]]. Moreover, simple isolated surface defects such as a groove, a slit or a corrugation on an otherwise planar surface provides a mechanism by which free-space radiation and SPs can exchange energy and hence couple.&lt;br /&gt;
&lt;br /&gt;
==Dispersion relation==&lt;br /&gt;
[[File:Coordinates.png|thumb|Figure 3: Coordinate system for 2 material interface]]&lt;br /&gt;
The electric field of a propagating electromagnetic wave can be expressed &lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;E= E_{0}\exp[i(k_{x} x + k_{z} z -\omega t)]\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;k&#039;&#039; is the [[wavenumber|wave number]] and ω is the frequency of the wave. By solving [[Maxwell&#039;s equations]] for the [[electromagnetic wave]] at an interface between two materials with relative [[Permitivity|dielectric functions]] &#039;&#039;ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039; and &#039;&#039;ε&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039; (see figure 3) with the appropriate continuity relation the boundary conditions are&amp;lt;ref name=&amp;quot;Raether&amp;quot;&amp;gt;{{cite book |last=Raether |first=Heinz |year=1988 |title=Surface Plasmons on Smooth and Rough Surfaces and on Gratings |location=New York |publisher=Springer-Verlag |isbn=3540173633| series=Springer Tracts in Modern Physics &#039;&#039;&#039;111&#039;&#039;&#039;}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;M.G. Cottam&amp;quot;&amp;gt;{{cite book |last=Cottam |first=Michael G. |year=1989 |title=Introduction to Surface and Superlattice Excitations |location=New York |publisher=Cambridge University Press |isbn=0750305886}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{k_{z1}}{\varepsilon_1} + \frac{k_{z2}}{\varepsilon_2} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;k_{x}^2+k_{zi}^2=\varepsilon_i \left(\frac{\omega}{c}\right)^2 \qquad i=1,2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;c&#039;&#039; is the [[speed of light]] in a vacuum, and &#039;&#039;k&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt;&#039;&#039; is same for both media at the interface for a surface wave. Solving these two equations, the dispersion relation for a wave propagating on the surface is&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;k_{x}=\frac{\omega}{c} \left(\frac{\varepsilon_1\varepsilon_2}{ \varepsilon_1+\varepsilon_2}\right)^{1/2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[File:Dispersion Relationship.png|thumb|Figure 4: Dispersion curve for surface plasmon polaritons. At low &#039;&#039;k&#039;&#039;, the surface plasmon curve (red) approaches the photon curve (blue)]]&lt;br /&gt;
In the [[Free_electron_model#Dielectric_function_of_the_electron_gas|free electron model of an electron gas]], which neglects attenuation, the metallic dielectric function is&amp;lt;ref&amp;gt;{{cite book |last=Kittel |first=Charles |authorlink=Charles Kittel |year=1996 |title=Introduction to Solid State Physics |edition= 8th |location= Hoboken, NJ |publisher=John Wiley &amp;amp; Sons |isbn=0-471-41526-X}}&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\varepsilon(\omega)=1-\frac{\omega_{P}^2}{\omega^2},&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where the bulk plasma frequency in SI units is &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\omega_{P}=\sqrt{\frac{n e^2}{{\varepsilon_0}m^*}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;n&#039;&#039; is the electron density, &#039;&#039;e&#039;&#039; is the [[Electron charge|charge]] of the electron, &#039;&#039;m&#039;&#039;&amp;lt;sup&amp;gt;*&amp;lt;/sup&amp;gt; is the [[Effective mass (solid-state physics)|effective mass]] of the electron and &amp;lt;math&amp;gt;{\varepsilon_0}&amp;lt;/math&amp;gt; is the permittivity of free-space. The [[Dispersion (optics)|dispersion]] relation is plotted in Figure 4. At low &#039;&#039;k&#039;&#039;, the SPP behaves like a photon, but as &#039;&#039;k&#039;&#039; increases, the dispersion relation bends over and reaches an [[asymptotic limit]] called the &amp;quot;surface plasma frequency&amp;quot;. Since the dispersion curve lies to the right of the light line, &#039;&#039;ω = k·c&#039;&#039;, the SPP has a shorter wavelength than free-space radiation such that the out-of-plane component of the SPP wavevector is purely imaginary and exhibits evanescent decay. The surface plasma frequency is the asymptote of this curve, and is given by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\omega_{SP}=\omega_P/\sqrt{1+\varepsilon_2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In the case of air, this result simplifies to &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\omega_{SP}=\omega_P/\sqrt{2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If we assume that &#039;&#039;ε&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039; is real and &#039;&#039;ε&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039;&#039; &amp;gt; 0, then it must be true that &#039;&#039;ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&#039; &amp;lt; 0, a condition which is satisfied in metals. Electromagnetic waves passing through a metal experience damping due to Ohmic losses and electron-core interactions. These effects show up in as an imaginary component of the [[dielectric function]]. The dielectric function of a metal is expressed ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt; = ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039; + i·ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;quot; where ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039; and ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;quot; are the real and imaginary parts of the dielectric function, respectively. Generally |ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;| &amp;gt;&amp;gt; ε&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&amp;quot; so the wavenumber can be expressed in terms of its real and imaginary components as&amp;lt;ref name=&amp;quot;Raether&amp;quot;/&amp;gt; &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;k_{x}=k_{x}&#039;+i k_{x}&#039;&#039;=\left[\frac{\omega}{c} \left( \frac{\varepsilon_1&#039; \varepsilon_2}{\varepsilon_1&#039; + \varepsilon_2}\right)^{1/2}\right] + i \left[\frac{\omega}{c} \left( \frac{\varepsilon_1&#039; \varepsilon_2}{\varepsilon_1&#039; + \varepsilon_2}\right)^{3/2} \frac{\varepsilon_1&#039;&#039;}{2(\varepsilon_1&#039;)^2}\right].&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The wave vector gives us insight into physically meaningful properties of the electromagnetic wave such as its spatial extent and coupling requirements for wave vector matching.&lt;br /&gt;
&lt;br /&gt;
==Propagation length and skin depth==&lt;br /&gt;
As an SPP propagates along the surface, it loses energy to the metal due to absorption. The intensity of the surface plasmon decays with the square of the [[electric field]], so at a distance &#039;&#039;x&#039;&#039;, the intensity has decreased by a factor of exp[-2k&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt;&amp;quot;x]. The propagation length is defined as the distance for the SPP intensity to decay by a factor of &#039;&#039;1/e&#039;&#039;. This condition is satisfied at a length&amp;lt;ref name=&amp;quot;Homola&amp;quot;&amp;gt;{{cite book |last=Homola |first=Jirí |year=2006 |title=Surface Plasmon Resonance Based Sensors. Springer Series on Chemical Sensors and Biosensors, &#039;&#039;&#039;4&#039;&#039;&#039;|location=Berlin |publisher=Springer-Verlag|isbn=3-540-33918-3}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;L=\frac{1}{2 k_{x}&#039;&#039;}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Likewise, the electric field falls off evanescently perpendicular to the metal surface. At low frequencies, the SPP penetration depth into the metal is commonly approximated using the [[skin depth]] formula. In the dielectric, the field will fall off far more slowly. The decay lengths in the metal and dielectric medium can be expressed as&amp;lt;ref name=&amp;quot;Homola&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;z_{i}=\frac{\lambda}{2 \pi} \left(\frac{|\varepsilon_1&#039;|+\varepsilon_2}{\varepsilon_i^2} \right)^{1/2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;i&#039;&#039; indicates the medium of propagation. SPPs are very sensitive to  slight perturbations within the skin depth and because of this, SPPs are often used to probe inhomogeneities of a surface.&lt;br /&gt;
&lt;br /&gt;
==Animations==&lt;br /&gt;
&amp;lt;gallery heights=&amp;quot;220px&amp;quot; widths=&amp;quot;400px&amp;quot; perrow=&amp;quot;2&amp;quot;&amp;gt;&lt;br /&gt;
File:SPP silver-air interface 370nm.gif|The [[electric field]] (E-field) of an SPP at the silver-air interface, at the frequency where the free-space wavelength is 370nm. The animation shows how the E-field varies over an optical cycle. The [[permittivity]] of silver at this frequency is {{nowrap|(-2.6 + 0.6i)}}. The picture is {{nowrap|(0.3 × 370nm)}} across horizontally; the SPP wavelength is much smaller than the free-space wavelength.&lt;br /&gt;
&lt;br /&gt;
File:SPP silver-air interface 10um.gif|The E-field of an SPP at the silver-air interface, at a much lower frequency corresponding to a free-space wavelength of 10μm. At this frequency, the silver behaves approximately as a [[perfect electric conductor]], and the SPP is called a [[surface wave|Sommerfeld Zenneck wave]], with almost the same wavelength as the free-space wavelength. The permittivity of silver at this frequency is {{nowrap|(-2700 + 1400i)}}. The picture is {{nowrap|(0.6 × 10μm)}} across horizontally.&lt;br /&gt;
&amp;lt;/gallery&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Experimental applications==&lt;br /&gt;
Nanofabricated systems that exploit SPPs demonstrate potential for designing and controlling the propagation of [[light]] in matter. In particular, SPPs can be used to channel light efficiently into [[nanometer]] scale volumes, leading to direct modification of [[Normal mode|resonate frequency dispersion]] properties (substantially shrinking the wavelength of light and the speed of light pulses for example), as well as field enhancements suitable for enabling strong interactions with [[nonlinear metamaterials|nonlinear materials]]. The resulting enhanced sensitivity of light to external parameters (for example, an applied electric field or the dielectric constant of an adsorbed molecular layer) shows great promise for applications in sensing and switching.&lt;br /&gt;
&lt;br /&gt;
Current research is focused on the design, fabrication, and experimental characterization of novel components for measurement and communications based on nanoscale plasmonic effects. These devices include ultra-compact plasmonic interferometers for applications such as [[biosensing]], optical positioning and optical switching, as well as the individual building blocks (plasmon source, waveguide and detector) needed to integrate a high-bandwidth, infrared-frequency plasmonic communications link on a silicon chip.&lt;br /&gt;
&lt;br /&gt;
In addition to building functional devices based on SPPs, it appears feasible to exploit the dispersion characteristics of SPPs traveling in confined metallo-dielectric spaces to create photonic materials with artificially tailored bulk optical characteristics, otherwise known as &#039;&#039;[[photonic metamaterials|metamaterials]]&#039;&#039;.&amp;lt;ref name=nanoplasmonics&amp;gt;&lt;br /&gt;
{{cite web&lt;br /&gt;
  | last =NIST researchers &lt;br /&gt;
  | first =Nanofabrication Research Group  &lt;br /&gt;
  | title =Nanoplasmonics&lt;br /&gt;
  | publisher =National Institute of Science and Technology &lt;br /&gt;
  | date = &lt;br /&gt;
  | url =http://www.nist.gov/cnst/nrg/nanoplasmonics.cfm&lt;br /&gt;
  | format =Online &lt;br /&gt;
  | accessdate =2011-02-15}} &lt;br /&gt;
*{{NIST-PD|article=Nanoplasmonics|url=http://www.nist.gov/cnst/nrg/nanoplasmonics.cfm}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The excitation of SPPs is frequently used in an experimental technique known as [[surface plasmon resonance]] (SPR). In SPR, the maximum excitation of surface plasmons are detected by monitoring the reflected power from a prism coupler as a function of incident angle or [[wavelength]]. This technique can be used to observe [[nanometer]] changes in thickness, density fluctuations, or molecular absorption.&lt;br /&gt;
&lt;br /&gt;
[[Surface plasmon]]-based circuits, including both SPPs and [[localized plasmon resonance]]s, have been proposed as a means of overcoming the size limitations of photonic circuits for use in high performance data processing nano devices.&amp;lt;ref&amp;gt;{{cite journal|doi=10.1126/science.1114849|title=Plasmonics: Merging Photonics and Electronics at Nanoscale Dimensions|year=2006|last1=Ozbay|first1=E.|journal=Science|volume=311|issue=5758|pages=189–93|pmid=16410515|bibcode = 2006Sci...311..189O }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The ability to dynamically control the plasmonic properties of materials in these nano-devices is key to their development. A new approach that uses plasmon-plasmon interactions has been demonstrated recently. Here the bulk plasmon resonance is induced or suppressed to manipulate the propagation of light.&amp;lt;ref&amp;gt;{{cite journal|doi=10.1088/0957-4484/23/44/444004|title=Plasmon–plasmon interaction: Controlling light at nanoscale|year=2012|last1=Akimov|first1=Yu A|last2=Chu|first2=H S|journal=Nanotechnology|volume=23|issue=44|pages=444004|pmid=23080049}}&amp;lt;/ref&amp;gt; This approach has been shown to have a high potential for nanoscale light manipulation and the development of a fully CMOS- compatible electro-optical plasmonic modulator.&lt;br /&gt;
&lt;br /&gt;
CMOS compatible electro-optic plasmonic modulators will be key components in chip-scale photonic circuits.&amp;lt;ref&amp;gt;{{cite journal|author=Wenshan Cai, Justin S. White, and Mark L. Brongersma|doi=10.1021/nl902701b|title=Compact, High-Speed and Power-Efficient Electrooptic Plasmonic Modulators|year=2009|journal=Nano Letters|volume=9|issue=12|pages=4403–11|pmid=19827771|bibcode = 2009NanoL...9.4403C }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In [[surface second harmonic generation]], the second harmonic signal is proportional to the square of the electric field. The electric field is stronger at the interface because of the surface plasmon resulting in a [[Nonlinear optics|non-linear optical effect]].  This larger signal is often exploited to produce a stronger second harmonic signal.&amp;lt;ref&amp;gt;{{cite journal|author=V. K. Valev|doi=10.1021/la302485c|title=Characterization of Nanostructured Plasmonic Surfaces with Second Harmonic Generation|year=2012|journal=Langmuir|volume=28|issue=44|pages=15454–15471}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The wavelength and intensity of the plasmon-related absorption and emission peaks are affected by molecular adsorption that can be used in molecular sensors. For example, a fully operational prototype device detecting casein in milk has been fabricated. The device is based on monitoring changes in plasmon-related absorption of light by a gold layer.&amp;lt;ref&amp;gt;{{cite journal|doi=10.1016/j.stam.2006.12.010|format=free download pdf|title=A localized surface plasmon resonance based immunosensor for the detection of casein in milk|year=2007|author=Minh Hiep, Ha|journal=Science and Technology of Advanced Materials|volume=8|pages=331|last2=Endo|first2=Tatsuro|last3=Kerman|first3=Kagan|last4=Chikae|first4=Miyuki|last5=Kim|first5=Do-Kyun|last6=Yamamura|first6=Shohei|last7=Takamura|first7=Yuzuru|last8=Tamiya|first8=Eiichi|bibcode = 2007STAdM...8..331M|issue=4 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Effects of roughness==&lt;br /&gt;
In order to understand the effect of roughness on SPPs, it is beneficial to first understand how a SPP is coupled by a [[Diffraction grating|grating]] [[#fig2anchor|Figure2]]. When a photon is incident on a surface, the wave vector of the photon in the dielectric material is smaller than that of the SPP. In order for the photon to couple into a SPP, the wave vector must increase by &amp;lt;math&amp;gt;\Delta k = k_{SP}- k_{x, \text{photon}}&amp;lt;/math&amp;gt;. The grating [[harmonics]] of a periodic grating provide additional momentum parallel to the supporting interface to match the terms.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;k_{SPP}=k_{x, \text{photon}} \pm n\ k_\text{grating}=\frac{\omega}{c} \sin{\theta_0} \pm n \frac{2\pi}{a}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;k_\text{grating}&amp;lt;/math&amp;gt; is the wave vector of the grating, &amp;lt;math&amp;gt;\theta_0&amp;lt;/math&amp;gt; is the angle of incidence of the incoming photon, &#039;&#039;a&#039;&#039; is the grating period, and &#039;&#039;n&#039;&#039; is an integer. &lt;br /&gt;
&lt;br /&gt;
Rough surfaces can be thought of as the [[Superposition principle|superposition]] of many gratings of different periodicities. Kretschmann proposed&amp;lt;ref name=&amp;quot;Kretschmann1&amp;quot;&amp;gt;{{de icon}} {{cite journal |last=Kretschmann |first=E. |date=April 1974 |title=Die Bestimmung der Oberflächenrauhigkeit dünner Schichten durch Messung der Winkelabhängigkeit der Streustrahlung von Oberflächenplasmaschwingungen |journal=[[Optics Communications]] |volume=10 |issue=4 |pages= 353–356 |doi=10.1016/0030-4018(74)90362-9|bibcode = 1974OptCo..10..353K }}&amp;lt;/ref&amp;gt; that a statistical [[correlation function]] be defined for a rough surface&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;G(x,y)=\frac{1}{A}\int_A z(x&#039;,y&#039;)\ z(x&#039;-x,y&#039;-y)\, dx&#039;\, dy&#039;&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;z(x,y)&amp;lt;/math&amp;gt; is the height above the mean surface height at the position &amp;lt;math&amp;gt;(x,y)&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt; is the area of integration. Assuming that the statistical correlation function is [[Gaussian function|Gaussian]] of the form&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;G(x,y)=\delta^2\exp\left(-\frac{r^2}{\sigma^2}\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\delta&amp;lt;/math&amp;gt; is the [[root mean square]] height, &amp;lt;math&amp;gt;r&amp;lt;/math&amp;gt; is the distance from the point &amp;lt;math&amp;gt;(x,y)&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt; is the correlation length, then the [[Fourier transform]] of the correlation function is&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;|s(k_\text{surf})|^2=\frac{1}{4 \pi} \sigma^2 \delta^2 \exp \left( - \frac{\sigma^2 k_\text{surf}^2}{4}\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;s&amp;lt;/math&amp;gt; is a measure of the amount of each [[spatial frequency]] &amp;lt;math&amp;gt; k_\text{surf}&amp;lt;/math&amp;gt; which help couple photons into a surface plasmon. &lt;br /&gt;
&lt;br /&gt;
If the surface only has one Fourier component of roughness (i.e. the surface profile is sinusoidal), then the &amp;lt;math&amp;gt;s&amp;lt;/math&amp;gt; is discrete and exists only at &amp;lt;math&amp;gt;k=\frac{2\pi}{a}&amp;lt;/math&amp;gt;, resulting in a single narrow set of angles for coupling. If the surface contains many Fourier components, then coupling becomes possible at multiple angles. For a random surface, &amp;lt;math&amp;gt;s&amp;lt;/math&amp;gt; becomes continuous and the range of coupling angles broadens.&lt;br /&gt;
&lt;br /&gt;
As stated earlier, SPPs are non-radiative. When a SPP travels along a rough surface, it usually becomes radiative due to scattering. The Surface Scattering Theory of light suggests that the scattered intensity &amp;lt;math&amp;gt;dI&amp;lt;/math&amp;gt; per [[solid angle]] &amp;lt;math&amp;gt;d \Omega&amp;lt;/math&amp;gt; per incident intensity &amp;lt;math&amp;gt;I_{0}&amp;lt;/math&amp;gt; is&amp;lt;ref name=&amp;quot;Kretschmann2&amp;quot;&amp;gt;{{cite journal |last=Kretschmann |first=E. |year=1972 |title=The angular dependence and the polarisation of light emitted by surface plasmons on metals due to roughness |journal=Optics Communications |volume=5 |issue=5 |pages= 331–336 |doi=10.1016/0030-4018(72)90026-0 |bibcode = 1972OptCo...5..331K }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{dI}{ d \Omega\ I_{0}}=\frac{4 \sqrt{\varepsilon_{0}}}{\cos{\theta_0}}\frac{\pi^4}{\lambda^4}|t_{012}^p|^2 \ |W|^2 |s(k_\text{surf})|^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;|W|^2&amp;lt;/math&amp;gt; is the radiation pattern from a single [[dipole]] at the metal/dielectric interface. If surface plasmons are excited in the Kretschmann geometry and the scattered light is observed in the plane of incidence (Fig. 4), then the dipole function becomes&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;|W|^2=A(\theta,|\varepsilon_{1}|)\ \sin^2{\psi} \ [(1+\sin^2 \theta /|\varepsilon_1|)^{1/2} - \sin{\theta}]^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; A(\theta,|\varepsilon_1|) = \frac{|\varepsilon_1|+1}{|\varepsilon_1|-1} \frac{4}{1+\tan{\theta}/| \varepsilon_1|}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\psi&amp;lt;/math&amp;gt; is the polarization angle and &amp;lt;math&amp;gt;\theta&amp;lt;/math&amp;gt; is the angle from the &#039;&#039;z&#039;&#039;-axis in the &#039;&#039;xz&#039;&#039;-plane. Two important consequences come out of these equations. The first is that if &amp;lt;math&amp;gt;\psi=0&amp;lt;/math&amp;gt; (s-polarization), then &amp;lt;math&amp;gt;|W|^2=0&amp;lt;/math&amp;gt; and the scattered light &amp;lt;math&amp;gt;\frac{dI}{ d \Omega\ I_{0}}=0&amp;lt;/math&amp;gt;. Secondly, the scattered light has a measurable profile which is readily correlated to the roughness.  This topic is treated in greater detail in reference.&amp;lt;ref name=&amp;quot;Kretschmann2&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Surface plasmon]]&lt;br /&gt;
* [[Surface plasmon resonance]]&lt;br /&gt;
* [[Plasmonic lens]]&lt;br /&gt;
* [[Superlens]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
&lt;br /&gt;
==Further reading==&lt;br /&gt;
*{{cite journal|last1=Ebbesen|doi=10.1038/35570|first1=T. W.|last2=Lezec|first2=H. J.|last3=Ghaemi|first3=H. F.|last4=Thio|first4=T.|last5=Wolff|first5=P. A.|title=Extraordinary optical transmission through sub-wavelength hole arrays|year=1998|page=667|volume=391|journal=Nature|url=http://arep.med.harvard.edu/pdf/Ebbsen98.pdf|bibcode = 1998Natur.391..667E|issue=6668}}&lt;br /&gt;
*{{cite journal|last1=Hendry|doi=10.1103/PhysRevLett.100.123901|first1=E.|last2=Garcia-Vidal|first2=F.|last3=Martin-Moreno|first3=L.|last4=Rivas|first4=J.|last5=Bonn|first5=M.|last6=Hibbins|first6=A.|last7=Lockyear|first7=M.|title=Optical Control over Surface-Plasmon-Polariton-Assisted THz Transmission through a Slit Aperture|pmid=18517865|year=2008|page=123901|issue=12|volume=100|journal=Physical Review Letters |url=http://shannon.ex.ac.uk/research/emag/pubs/pdf/Hendry_PRL_2008.pdf|bibcode=2008PhRvL.100l3901H}} Free PDF download.&lt;br /&gt;
*{{cite journal|last1=Barnes|first1=William L.|last2=Dereux|first2=Alain|last3=Ebbesen|first3=Thomas W.|title=Surface plasmon subwavelength optics|doi=10.1038/nature01937|pmid=12917696|year=2003|pages=824|issue=6950|volume=424|journal=Nature&lt;br /&gt;
|url=http://access.ex.ac.uk/research/emag/wlb/nature_2003_424_824.pdf|bibcode = 2003Natur.424..824B }} Free PDF download.&lt;br /&gt;
*{{cite journal|last1 =Pitarke|first1 =J M|last2 =Silkin|first2 =V M|last3 =Chulkov|first3 =E V|last4 =Echenique|first4 =P M|doi =10.1088/0034-4885/70/1/R01|title =Theory of surface plasmons and surface-plasmon polaritons|year =2007|pages =1|volume =70|journal =Reports on Progress in Physics&lt;br /&gt;
|url =http://dipc.ehu.es/etxenike/admin/documentos/archivos/publicaciones/307RPP2007.pdf|arxiv = cond-mat/0611257 |bibcode = 2007RPPh...70....1P }} Free PDF download.&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
*{{Cite web&lt;br /&gt;
  | last =White &lt;br /&gt;
  | first =Justin  &lt;br /&gt;
  | authorlink = &lt;br /&gt;
  | coauthors = &lt;br /&gt;
  | title =Surface Plasmon Polaritons &lt;br /&gt;
  | work = &lt;br /&gt;
  | publisher =[[Stanford University]]. Physics department &lt;br /&gt;
  | date =March 19, 2007 &lt;br /&gt;
  | url =http://large.stanford.edu/courses/2007/ap272/white1/ &lt;br /&gt;
  | format =Online &lt;br /&gt;
  | doi = &lt;br /&gt;
  | accessdate =}} &amp;quot;&#039;&#039;Submitted as coursework for AP272. Winter 2007&#039;&#039;&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Surface Plasmon Polaritons}}&lt;br /&gt;
[[Category:Optics]]&lt;br /&gt;
[[Category:Engineering]]&lt;br /&gt;
[[Category:Metamaterials]]&lt;br /&gt;
[[Category:Condensed matter physics]]&lt;/div&gt;</summary>
		<author><name>131.111.204.168</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Minkowski%27s_second_theorem&amp;diff=27882</id>
		<title>Minkowski&#039;s second theorem</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Minkowski%27s_second_theorem&amp;diff=27882"/>
		<updated>2013-08-30T14:02:10Z</updated>

		<summary type="html">&lt;p&gt;131.111.24.214: /* Statement of the theorem */ Replaced the Rs with \mathbb{R}s.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[mathematics]], the &#039;&#039;&#039;perpendicular bisector construction&#039;&#039;&#039; is a construction which produces a new [[quadrilateral]] from a given quadrilateral using the perpendicular bisectors to the sides of the former quadrilateral. This construction arises very naturally and has been considered by many authors over the years.&lt;br /&gt;
&lt;br /&gt;
==Definition of the construction==&lt;br /&gt;
Suppose that the [[vertex (geometry)|vertices]] of the [[quadrilateral]] &amp;lt;math&amp;gt; Q &amp;lt;/math&amp;gt; are given by &amp;lt;math&amp;gt; Q_1,Q_2,Q_3,Q_4  &amp;lt;/math&amp;gt;. Let &amp;lt;math&amp;gt; b_1,b_2,b_3,b_4 &amp;lt;/math&amp;gt; be the perpendicular bisectors of sides &amp;lt;math&amp;gt; Q_1Q_2,Q_2Q_3,Q_3Q_4,Q_4Q_1 &amp;lt;/math&amp;gt; respectively. Then their intersections &amp;lt;math&amp;gt; Q_i^{(2)}=b_{i+2}b_{i+3} &amp;lt;/math&amp;gt;, with subscripts considered modulo 4, form the consequent quadrilateral &amp;lt;math&amp;gt; Q^{(2)} &amp;lt;/math&amp;gt;. The construction is then iterated on &amp;lt;math&amp;gt; Q^{(2)} &amp;lt;/math&amp;gt; to produce &amp;lt;math&amp;gt; Q^{(3)} &amp;lt;/math&amp;gt; and so on.&lt;br /&gt;
[[File:PerpendicularBisectorConstruction.svg|thumb|360px|First iteration of the perpendicular bisector construction]]&lt;br /&gt;
&lt;br /&gt;
An equivalent construction can be obtained by letting the vertices of &amp;lt;math&amp;gt; Q^{(i+1)} &amp;lt;/math&amp;gt; be the [[circumcenter]]s of the 4 triangles formed by selecting combinations of 3 vertices of &amp;lt;math&amp;gt; Q^{(i)} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Properties==&lt;br /&gt;
1. If &amp;lt;math&amp;gt; Q^{(1)} &amp;lt;/math&amp;gt; is not cyclic, then &amp;lt;math&amp;gt; Q^{(2)} &amp;lt;/math&amp;gt; is not degenerate.&amp;lt;ref name=King&amp;gt;J. King, Quadrilaterals formed by perpendicular bisectors, in &#039;&#039;Geometry Turned On&#039;&#039;, (ed. J. King), MAA Notes 41, 1997, pp. 29–32.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
2. Quadrilateral &amp;lt;math&amp;gt; Q^{(2)} &amp;lt;/math&amp;gt; is never cyclic.&amp;lt;ref name=&amp;quot;King&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
3. Quadrilaterals &amp;lt;math&amp;gt; Q^{(1)} &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; Q^{(3)} &amp;lt;/math&amp;gt; are [[Homothety|homothetic]], and in particular, [[Similarity (geometry)|similar]].&amp;lt;ref name=Shephard&amp;gt;G. C. Shephard, The perpendicular bisector construction, &#039;&#039;Geom. Dedicata&#039;&#039;, 56 (1995) 75–84.&amp;lt;/ref&amp;gt; Quadrilaterals &amp;lt;math&amp;gt; Q^{(2)} &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; Q^{(4)} &amp;lt;/math&amp;gt; are also homothetic.&lt;br /&gt;
&lt;br /&gt;
3. The Perpendicular bisector construction can be reversed via [[isogonal conjugation]].&amp;lt;ref name=RadkoTsukerman&amp;gt;O. Radko and E. Tsukerman, The Perpendicular Bisector Construction, the Isoptic Point and the Simson Line of a Quadrilateral, &#039;&#039;Forum Geometricorum&#039;&#039; &#039;&#039;&#039;12&#039;&#039;&#039;: 161–189 (2012).&amp;lt;/ref&amp;gt; That is, given &amp;lt;math&amp;gt; Q^{(i+1)} &amp;lt;/math&amp;gt;, it is possible to construct &amp;lt;math&amp;gt; Q^{(i)} &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
4. Let &amp;lt;math&amp;gt; \alpha, \beta, \gamma, \delta &amp;lt;/math&amp;gt; be the angles of &amp;lt;math&amp;gt; Q^{(1)} &amp;lt;/math&amp;gt;. For every &amp;lt;math&amp;gt; i &amp;lt;/math&amp;gt;, the ratio of areas of &amp;lt;math&amp;gt; Q^{(i)} &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; Q^{(i+1)} &amp;lt;/math&amp;gt; is given by&amp;lt;ref name=&amp;quot;RadkoTsukerman&amp;quot; /&amp;gt;  &lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;text-align: center;&amp;quot;&amp;gt;&amp;lt;math&amp;gt; (1/4)(cot(\alpha)+cot(\gamma))(cot(\beta)+cot(\delta)). &amp;lt;/math&amp;gt;&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
5. If &amp;lt;math&amp;gt; Q^{(1)} &amp;lt;/math&amp;gt; is convex then the sequence of quadrilaterals &amp;lt;math&amp;gt; Q^{(1)}, Q^{(2)},\ldots &amp;lt;/math&amp;gt; converges to the [[Isoptic Point]] of &amp;lt;math&amp;gt; Q^{(1)} &amp;lt;/math&amp;gt;, which is also the Isoptic Point for every &amp;lt;math&amp;gt; Q^{(i)} &amp;lt;/math&amp;gt;. Similarly, if &amp;lt;math&amp;gt; Q^{(1)} &amp;lt;/math&amp;gt; is concave, then the sequence &amp;lt;math&amp;gt; Q^{(1)}, Q^{(0)}, Q^{(-1)},\ldots &amp;lt;/math&amp;gt; obtained by reversing the construction converges to the Isoptic Point of the &amp;lt;math&amp;gt; Q^{(i)} &amp;lt;/math&amp;gt;&#039;s.&amp;lt;ref name=&amp;quot;RadkoTsukerman&amp;quot; /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Motivating discussion==&lt;br /&gt;
The perpendicular bisector construction arises naturally in an attempt to find a replacement for the [[circumcenter]] of a quadrilateral in the case that it is noncyclic.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&amp;lt;!--- After listing your sources please cite them using inline citations and place them after the information they cite. Please see http://en.wikipedia.org/wiki/Wikipedia:REFB for instructions on how to add citations. ---&amp;gt;&lt;br /&gt;
* J. Langr, Problem E1050, &#039;&#039;Amer. Math. Monthly&#039;&#039;, 60 (1953) 551.&lt;br /&gt;
* V. V. Prasolov, &#039;&#039;Plane Geometry Problems&#039;&#039;, vol. 1 (in Russian), 1991; Problem 6.31.&lt;br /&gt;
* V. V. Prasolov, &#039;&#039;Problems in Plane and Solid Geometry&#039;&#039;, vol. 1 (translated by D. Leites), available at http://students.imsa.edu/~tliu/math/planegeo.eps.&lt;br /&gt;
* D. Bennett, Dynamic geometry renews interest in an old problem, in &#039;&#039;Geometry Turned On&#039;&#039;, (ed. J. King), MAA Notes 41, 1997, pp.&amp;amp;nbsp;25–28.&lt;br /&gt;
* J. King, Quadrilaterals formed by perpendicular bisectors, in &#039;&#039;Geometry Turned On&#039;&#039;, (ed. J. King), MAA Notes 41, 1997, pp.&amp;amp;nbsp;29–32.&lt;br /&gt;
* G. C. Shephard, The perpendicular bisector construction, &#039;&#039;Geom. Dedicata&#039;&#039;, 56 (1995) 75–84.&lt;br /&gt;
* A. Bogomolny, Quadrilaterals formed by perpendicular bisectors, &#039;&#039;Interactive Mathematics Miscellany and Puzzles&#039;&#039;, http://www.cut-the-knot.org/Curriculum/Geometry/PerpBisectQuadri.shtml.&lt;br /&gt;
*  B. Grünbaum, On  quadrangles  derived  from quadrangles—Part 3, &#039;&#039;Geombinatorics&#039;&#039; 7(1998), 88–94.&lt;br /&gt;
* O. Radko and E. Tsukerman, The Perpendicular Bisector Construction, the Isoptic Point and the Simson Line of a Quadrilateral, &#039;&#039;Forum Geometricorum&#039;&#039; &#039;&#039;&#039;12&#039;&#039;&#039;: 161–189 (2012).&lt;br /&gt;
&lt;br /&gt;
[[Category:Quadrilaterals]]&lt;/div&gt;</summary>
		<author><name>131.111.24.214</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Inertial_number&amp;diff=26883</id>
		<title>Inertial number</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Inertial_number&amp;diff=26883"/>
		<updated>2013-08-20T13:48:16Z</updated>

		<summary type="html">&lt;p&gt;131.111.16.74: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;Maxwell-Bloch equations&#039;&#039;&#039;, also called the &#039;&#039;&#039;optical Bloch equations&#039;&#039;&#039;, describe the dynamics of a [[two-state quantum system]] interacting with the electromagnetic mode of an optical resonator. They are analogous to (but not at all equivalent to) the [[Bloch equation]]s which describe the motion of the nuclear magnetic moment in an electromagnetic field. The equations can be derived either semiclassically or with the field fully quantized when certain approximations are made.&lt;br /&gt;
&lt;br /&gt;
==Semi-classical formulation==&lt;br /&gt;
The derivation of the semi-classical optical Bloch equations is nearly identical to solving the [[two-state quantum system]] (see the discussion there). However, usually one casts these equations into a density matrix form. The system we are dealing with can be described by the wave function: &lt;br /&gt;
:&amp;lt;math&amp;gt; \psi = c_g\psi_g + c_e\psi_e &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; \left|c_g\right|^2 + \left|c_e\right|^2 = 1 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The [[density matrix]] is &lt;br /&gt;
:&amp;lt;math&amp;gt; \rho = \begin{bmatrix}\rho_{ee} &amp;amp; \rho_{eg} \\ \rho_{ge} &amp;amp; \rho_{gg}\end{bmatrix} = \begin{bmatrix}c_e c_{e}^* &amp;amp; c_e c_{g}^* \\ c_g c_{e}^* &amp;amp; c_g c_{g}^* \end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(other conventions are possible; this follows the derivation in Metcalf (1999)).&amp;lt;ref name=&amp;quot;metcalf&amp;quot;&amp;gt;Metcalf, Harold. &#039;&#039;Laser Cooling and Trapping&#039;&#039; Springer 1999 pg. 24-&amp;lt;/ref&amp;gt; One can now solve the Heisenberg equation of motion, or translate the results from solving the Schrödinger equation into density matrix form. One arrives at the following equations, including spontaneous emission: &lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d \rho_{gg}}{dt} = \gamma \rho_{ee} + \frac{i}{2}(\Omega^* \bar \rho_{eg} - \Omega\bar \rho_{ge})&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d \rho_{ee}}{dt} = -\gamma \rho_{ee} + \frac{i}{2}(\Omega \bar \rho_{ge} - \Omega^*\bar \rho_{eg})&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{d \bar \rho_{ge}}{dt} = -\left( \frac{\gamma}{2} + i\delta \right) \bar \rho_{ge} + \frac{i}{2}\Omega^*(\rho_{ee} - \rho_{gg})&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d \bar \rho_{eg}}{dt} = - \left( \frac{\gamma}{2} - i\delta \right) \bar \rho_{eg} + \frac{i}{2}\Omega^*(\rho_{gg} - \rho_{ee})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In the derivation of these formulae it was explicitly assumed that spontaneous emission is described by an exponential decay of the coefficient &amp;lt;math&amp;gt;\rho_{eg}(t)&amp;lt;/math&amp;gt; with decay constant &amp;lt;math&amp;gt;\frac{\gamma}{2}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt;\Omega&amp;lt;/math&amp;gt; is the (generalized) [[Rabi frequency]], which is &lt;br /&gt;
:&amp;lt;math&amp;gt;\Omega = \sqrt{|\chi_{g,e}|^2 + \delta^2}&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\delta = \omega - \omega_{0}&amp;lt;/math&amp;gt; is the detuning and measures how far the light frequency, &amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt;, is from the transition, &amp;lt;math&amp;gt;\omega_{0}&amp;lt;/math&amp;gt;. &amp;lt;math&amp;gt; \chi_{g,e} = {\vec{d}_{g,e}\cdot\vec{E}_0 \over \hbar}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;\scriptstyle{\vec{d}_{g,e}}&amp;lt;/math&amp;gt; is the [[transition dipole moment]] for the &amp;lt;math&amp;gt;\scriptstyle{g \rightarrow e}&amp;lt;/math&amp;gt; transition and &amp;lt;math&amp;gt;\scriptstyle{\vec{E}_0 = \hat{\epsilon}E_0}&amp;lt;/math&amp;gt; is the [[vector (geometric)|vector]] [[electric field]] amplitude including the [[Polarization (waves)|polarization]].&lt;br /&gt;
&lt;br /&gt;
==Derivation from Cavity Quantum Electrodynamics==&lt;br /&gt;
{{Unreferenced section|date=July 2011}}&lt;br /&gt;
Beginning with the [[Jaynes-Cummings model|Jaynes-Cummings Hamiltonian]] under [[coherent state|coherent drive]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;H=\omega_c a^\dagger a + \omega_a \sigma^\dagger\sigma+ig(a^\dagger\sigma-a\sigma^\dagger)+iJ(a^\dagger e^{-i\omega_l t}-a e^{i\omega_l t})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt; a&amp;lt;/math&amp;gt; is the [[lowering operator]] for the cavity field, and &amp;lt;math&amp;gt; \sigma=\frac{1}{2}\left(\sigma_x - i\sigma_y\right) &amp;lt;/math&amp;gt; is the atomic lowering operator written as a combination of [[Pauli matrices]]. The time dependence can be removed by transforming the wavefunction according to &amp;lt;math&amp;gt; |\psi\rangle\rightarrow \operatorname{e}^{-i\omega_l t\left(a^\dagger a + \sigma^\dagger\sigma\right)}|\psi\rangle&amp;lt;/math&amp;gt;, leading to a transformed Hamiltonian&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;H=\Delta_c a^\dagger a + \Delta_a \sigma^\dagger\sigma+ig(a^\dagger\sigma-a\sigma^\dagger)+iJ( a^\dagger-a)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt; \Delta_i = \omega_i - \omega_l &amp;lt;/math&amp;gt;. As it stands now, the Hamiltonian has four terms. The first two are the self energy of the atom (or other two level system) and field. The third term is an energy conserving interaction term allowing the cavity and atom to exchange population and coherence. These three terms alone give rise to the Jaynes-Cummings ladder of dressed states, and the associated anharmonicity in the energy spectrum. The last term models coupling between the cavity mode and a classical field, i.e. a laser. The drive strength &amp;lt;math&amp;gt; J &amp;lt;/math&amp;gt; is given in terms of the power transmitted through the empty two-sided cavity as &amp;lt;math&amp;gt; J=\sqrt{2P(\Delta_c^2 + \kappa^2)/(\hbar\omega_c \kappa)} &amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;2\kappa&amp;lt;/math&amp;gt; is the cavity linewidth. This brings to light a crucial point concerning the role of dissipation in the operation of a laser or other cqed device; dissipation is the means by which the system (coupled atom/cavity) interacts with its environment. To this end, dissipation is included by framing the problem in terms of the master equation, where the last two terms are in the [[Lindblad superoperator|Lindblad form]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\dot{\rho}=-i[H,\rho] + 2\kappa\left(a\rho a^\dagger -\frac{1}{2}\left(a^\dagger a \rho + \rho a^\dagger a\right)\right) + 2\gamma\left(\sigma\rho &lt;br /&gt;
\sigma^\dagger -\frac{1}{2}\left(\sigma^\dagger \sigma\rho + \rho \sigma^\dagger \sigma\right)\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The equations of motion for the expectation values of the operators can be derived from the master equation by the formula &amp;lt;math&amp;gt; \langle\dot{O}\rangle = \operatorname{tr}\left(O\rho\right) &amp;lt;/math&amp;gt;. The equations of motion for &amp;lt;math&amp;gt; \langle a\rangle &amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt; \langle\sigma\rangle &amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt; \langle\sigma_z\rangle &amp;lt;/math&amp;gt;, the cavity field, atomic ground state population, and atomic inversion respectively, are&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d}{dt}\langle a \rangle = i\left(-\Delta_c \langle a \rangle - ig\langle \sigma\rangle - iJ\right) -\kappa \langle a \rangle &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d}{dt}\langle \sigma \rangle = i\left(-\Delta_a \langle \sigma \rangle - ig\langle a \sigma_z \rangle\right) -\gamma \langle \sigma \rangle &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d}{dt}\langle \sigma_z \rangle = -2g\left(\langle a^\dagger \sigma \rangle+\langle a \sigma^\dagger \rangle\right) -2\gamma \langle \sigma_z\rangle-2\gamma  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
At this point, we have produced three of an infinite ladder of coupled equations. As can be seen from the third equation, higher order correlations are necessary. The differential equation for the time evolution of &amp;lt;math&amp;gt;\langle a^\dagger \sigma \rangle &amp;lt;/math&amp;gt; will contain expectation values of higher order products of operators, thus leading to an infinite set of coupled equations. We heuristically make the approximation that the expectation value of a product of operators is equal to the product of expectation values of the individual operators. This is akin to assuming that the operators are uncorrelated, and is a good approximation in the classical limit. It turns out that the resulting equations give the correct qualitative behavior even in the single excitation regime. Additionally, to simplify the equations we make the following replacements&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle a \rangle = (\gamma/\sqrt{2} g)x &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle \sigma \rangle = -p/\sqrt{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle \sigma_z\rangle = -D  &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\Theta = \Delta_c/\kappa &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; C = g^2/2\kappa\gamma &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; y = \sqrt{2} g J/\kappa\gamma  &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; \Delta=\Delta_a/\gamma  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
And the Maxwell-Bloch equations can be written in their final form&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\dot{x}=\kappa\left(-2Cp+y-(i\Theta+1)x\right) &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\dot{p} = \gamma\left( -(1+i\Delta)p + xD\right)   &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\dot{D}=\gamma\left(2(1-D)-(x^*p+xp^*)\right) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Quantum mechanics]]&lt;br /&gt;
[[Category:Theoretical physics]]&lt;/div&gt;</summary>
		<author><name>131.111.16.74</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=E-folding&amp;diff=11225</id>
		<title>E-folding</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=E-folding&amp;diff=11225"/>
		<updated>2013-05-14T20:42:39Z</updated>

		<summary type="html">&lt;p&gt;131.111.184.92: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[physics]], &#039;&#039;&#039;Hamiltonian lattice gauge theory&#039;&#039;&#039; is a calculational approach to [[gauge theory]] and a special case of [[lattice gauge theory]] in which the space is discretized but time is not. The [[Hamiltonian_(quantum_mechanics)|Hamiltonian]] is then re-expressed as a function of degrees of freedom defined on a d-dimensional lattice.&lt;br /&gt;
&lt;br /&gt;
Following Wilson, the spatial components of the [[vector potential]] are replaced with [[Wilson line]]s over the edges, but the time component is associated with the vertices. However, the [[temporal gauge]] is often employed, setting the [[electric potential]] to zero. The [[eigenvalue]]s of the Wilson line [[operator (mathematics)|operator]]s U(e) (where e is the ([[oriented]]) edge in question) take on values on the [[Lie group]] G. It is assumed that G is [[compact group|compact]], otherwise we run into many problems. The conjugate operator to U(e) is the [[electric field]] E(e) whose eigenvalues take on values in the Lie algebra &amp;lt;math&amp;gt;\mathfrak{g}&amp;lt;/math&amp;gt;. The Hamiltonian receives contributions coming from the plaquettes (the magnetic contribution) and contributions coming from the edges (the electric contribution).&lt;br /&gt;
&lt;br /&gt;
Hamiltonian lattice gauge theory is exactly dual to a theory of [[spin network]]s. This involves using the [[Peter-Weyl theorem]]. In the spin network basis, the spin network states are [[eigenstate]]s of the operator &amp;lt;math&amp;gt;Tr[E(e)^2]&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
{{quantum-stub}}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*Hamiltonian formulation of Wilson&#039;s lattice gauge theories, [[John Kogut]] and [[Leonard Susskind]], &#039;&#039;Phys. Rev. D&#039;&#039; 11, 395&amp;amp;ndash;408 (1975)&lt;br /&gt;
&lt;br /&gt;
[[Category:Lattice models]]&lt;/div&gt;</summary>
		<author><name>131.111.184.92</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Reflective_subcategory&amp;diff=12744</id>
		<title>Reflective subcategory</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Reflective_subcategory&amp;diff=12744"/>
		<updated>2013-05-07T13:53:26Z</updated>

		<summary type="html">&lt;p&gt;131.111.185.88: fixed typo&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Originally, both [[Deutsche Bundesbahn]] and [[Deutsche Reichsbahn of the GDR|Deutsche Reichsbahn]] continued the classification system of the [[Deutsche Reichsbahn-Gesellschaft|Deutsche Reichsbahn (DRG)]] - see also a short overview of the [[Numbering scheme of the German railways|numbering system of the German railways]]. When [[International Union of Railways|UIC]] introduced a new classification system that could be processed by the computers of the late 1960s, DB did a major modification of their system, effective 1 January 1968. This system is still in use and now includes the engines of the former GDR railways as well. (See [[List of Deutsche Bahn AG locomotives and railbuses]] for a current list.)&lt;br /&gt;
&lt;br /&gt;
==Basics==&lt;br /&gt;
Since January 1, 1968, all vehicles are denoted by a seven-digit vehicle number. It consists of a three-digit class number, a three-digit serial number and a [[check digit]] separated by a dash. The check digit is calculated by multiplying the first six digits by 1 and 2 alternately, the difference of the result to the next multitude of ten is the check digit. The check digit is used to perform a cross-check to ensure the correct number, for example in computer systems.&lt;br /&gt;
&lt;br /&gt;
Series that contain more than 1,000 vehicles are assigned ascending numbers.&lt;br /&gt;
&lt;br /&gt;
The first number denotes the type of the vehicle, replacing the DRG convention of using letters to differentiate between the vehicle types.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
! Number || Letter(s) || Vehicle type&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 0 || &amp;amp;nbsp; || [[Steam locomotive]]s&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 1 || E || [[Electric locomotive]]s&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 2 || V || [[Diesel locomotive]]s&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 3 || K || Small [[Shunt (rail)|shunting]] locomotives&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 4 || ET || [[Electric multiple units]], not including battery powered&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 5 || ETA || Battery powered [[railcar]]s&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 6 || VT || [[Diesel multiple units]]&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 7 || &amp;amp;nbsp; || [[Railbus]]es and work vehicles&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 8 || ES, EB || Cab cars and accompanying cars to electric railcars&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 9 || VS, VB || Cab cars and accompanying cars to diesel railcars and railbuses&lt;br /&gt;
|} &lt;br /&gt;
&lt;br /&gt;
The letters of the DRG schema are not officially used any more since the introduction of computer numbers, however they can often be found in informal writing and spoken conversation. So if somebody is talking of an E110, they likely mean an E10 / 110, if a V216 is mentioned, it is likely the author is intending the V160 / 216.&lt;br /&gt;
 &lt;br /&gt;
Tenders are not assigned a number of their own, as they are regarded a part of the vehicle they are coupled to.&lt;br /&gt;
[[Cab car]]s and intermediate cars of [[multiple unit]]s receive the numbers 8 if they belong to an [[Electrical Multiple Unit|EMU]], 9 if they belong to a [[Diesel multiple unit|DMU]]. If another powered car or engine is present in the multiple unit, its serial number usually is offset by 500, but it is still assigned into the original class.&lt;br /&gt;
&lt;br /&gt;
For example, a two-car [[DB Class 628|Class 628]] DMU would look like:&lt;br /&gt;
* 628 210-7 (powered cab car)&lt;br /&gt;
* 928 210-4 (non-powered cab, hence 9 instead of 6)&lt;br /&gt;
&lt;br /&gt;
A [[DB Class 420|class 420]] commuter EMU, for example, would look like this:&lt;br /&gt;
* 420 210-1  (powered cab car)&lt;br /&gt;
* 421 210-2  (powered intermediate car)&lt;br /&gt;
* 420 710-7  (powered cab car, +500)&lt;br /&gt;
&lt;br /&gt;
===Example: 110&amp;amp;nbsp;494-2===&lt;br /&gt;
[[Image:Bahn Logo.jpg|thumb|Electric class 110 locomotive - 110 494-2]]&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
! colspan=&amp;quot;2&amp;quot; | Meaning of 110&amp;amp;nbsp;494-2&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;tt&amp;gt;110&amp;lt;/tt&amp;gt; || Class number &amp;lt;br&amp;gt; → first number (&amp;lt;tt&amp;gt;1&amp;lt;/tt&amp;gt;) meaning [[electric locomotive]]&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;tt&amp;gt;494&amp;lt;/tt&amp;gt; || Serial number&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;tt&amp;gt;2&amp;lt;/tt&amp;gt; || Check digit&lt;br /&gt;
|- &lt;br /&gt;
! colspan=&amp;quot;2&amp;quot; | How to calculate the check digit&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;math&amp;gt;1\!+\!0\!+\!9\,=\,10&amp;lt;/math&amp;gt; || Add 1st, 3rd and 5th number.&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;math&amp;gt;2\!\cdot\!1\,+\,2\!\cdot\!4\,+\,2\!\cdot\!4\,=\,18&amp;lt;/math&amp;gt; || Digit sum of the double of 2nd, 4th and 6th number.&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;math&amp;gt;10\!+\!18\,=\,28&amp;lt;/math&amp;gt; || Add both results.&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;math&amp;gt;30\!-\!28\,=\,2&amp;lt;/math&amp;gt; || Difference of the result to the next&amp;lt;br&amp;gt; multiple of ten is the check digit.&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
| &amp;lt;math&amp;gt;\,2&amp;lt;/math&amp;gt; || check digit&lt;br /&gt;
|- valign=&amp;quot;top&amp;quot;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Steam locomotives==&lt;br /&gt;
See also: [[DRG locomotive classification]] for the origins of the system.&lt;br /&gt;
&lt;br /&gt;
The number &#039;&#039;&#039;0&#039;&#039;&#039; was assigned to steam locomotives, as their end of duty was already foreseeable. The schematics are largely derivative of the DRG system of classification, therefore like in the older system the class numbers were grouped by locomotive types:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
! Number || Vehicle types&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 001–019 || [[Express train]] [[tender locomotive]]s&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 020–039 || Other [[Passenger train]] tender locomotives&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 040–059 || [[Freight train]] tender locomotives&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 060–079 || Passenger train [[tank locomotives]]&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 080–096 || Freight train tank locomotives&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 097|| [[Rack railway|Rack]] locomotives &amp;lt;small&amp;gt;(in theory only - none were left by 1968)&amp;lt;/small&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 098 || &#039;&#039;Lokalbahn&#039;&#039; (branch line) engines&lt;br /&gt;
|-&lt;br /&gt;
| align=&amp;quot;center&amp;quot; | 099 || [[narrow gauge railway|narrow gauge]] locomotives&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
[[Image:Class 55 2967 Front.jpg|right|thumb|200px|Class 55 engine 2967 in late 1950s West Germany.]]&lt;br /&gt;
Steam locomotives that had been converted to oil fuelling received separate class numbers from their coal-fuelled counterparts, e.&amp;amp;nbsp;g. oil-fuelled units from the old [[DRG Class 44|class 44]] were assigned to class 043 while coal-fuelled ones were assigned to class 044 under the new numbering plan. The [[DRB Class 50]] (with originally more than 3,000 units, of which DB still had more than 1,000 by the end of 1967) gave rise to BR 050, 051, 052 and 053. &lt;br /&gt;
&lt;br /&gt;
A noteworthy change from the old system was that four-digit engine numbers were no longer possible. Locomotives with such a number would either be put into an overflow class (e.&amp;amp;nbsp;g. &#039;&#039;50&amp;amp;nbsp;3097&#039;&#039; became &#039;&#039;053&amp;amp;nbsp;097-2&#039;&#039;) or have their number abbreviated to three digits. The latter solution could lead to number conflicts in cases where the original (sub)class had comprised more than 1,000 units. These were dealt with by adjusting one of the numbers involved, e.&amp;amp;nbsp;g., &#039;&#039;38&amp;amp;nbsp;3711&#039;&#039; became &#039;&#039;038&amp;amp;nbsp;711-8&#039;&#039; while &#039;&#039;38&amp;amp;nbsp;1711&#039;&#039; became &#039;&#039;038&amp;amp;nbsp;710-0&#039;&#039;. This also means that for some classes it is not possible to reconstruct the old number from the new one in a purely systematic way.&lt;br /&gt;
&lt;br /&gt;
The last steam locomotives in the [[Deutsche Bundesbahn]] were decommissioned on 26 October 1977 at &#039;&#039;Rheine und Emden&#039;&#039; locomotive depot (&#039;&#039;[[Bahnbetriebswerk]]&#039;&#039; or &#039;&#039;Bw&#039;&#039;). These were the 043 903, 043 315 and 043 196 .&lt;br /&gt;
&lt;br /&gt;
==Electric engines==&lt;br /&gt;
Electric engines were considered the most important method of traction, and hence were assigned the number &#039;&#039;&#039;1&#039;&#039;&#039;.&lt;br /&gt;
They usually were relabelled by replacing the letter &amp;quot;E&amp;quot; with the number &amp;quot;1&amp;quot;.&lt;br /&gt;
For example, the &#039;&#039;[[Einheits-Elektrolokomotive]]n&#039;&#039; were relabelled from E&amp;amp;nbsp;40 into 140, E&amp;amp;nbsp;10 into 110 and E&amp;amp;nbsp;10.12 into 112.&lt;br /&gt;
&lt;br /&gt;
==Diesel engines==&lt;br /&gt;
[[Image:V200 048.jpg|right|thumb|140px|V200 No. 048 in West Germany, circa 1961.]]&lt;br /&gt;
In the pre-1968 scheme, diesel engines were assigned the letter &amp;quot;V&amp;quot; (as in the German term &#039;&#039;Verbrennungsmotor&#039;&#039; for combustion engine). The old numbers were directly proportional with the engine power, so that two- and three-digit codes existed. Two-digit codes were transposed one by one (Examples: Class V60 became  [[DB Class 260|Class&amp;amp;nbsp;260]], Class&amp;amp;nbsp;V80 became [[DB Class 280|Class 280]]). Three digit codes generally lost their last digit (V&amp;amp;nbsp;160 became [[DBAG Class 210, 215 - 218, 219 old|DB Class 216]]). Variants of the previously same class were also assigned individual subclasses, the  [[DBAG class 210, 215 - 218, 219 old|V&amp;amp;nbsp;160 family]], consisting of V&amp;amp;nbsp;160, V&amp;amp;nbsp;160&amp;amp;nbsp;long (V&amp;amp;nbsp;160.3, V&amp;amp;nbsp;168), V&amp;amp;nbsp;162, V&amp;amp;nbsp;164 and V&amp;amp;nbsp;169 were assigned the numbers 210, 215, 216, 217, 218 and 219, for example.)&lt;br /&gt;
&lt;br /&gt;
==Small locomotives==&lt;br /&gt;
Small shunting locomotives were assigned the number &amp;quot;3&amp;quot;. The second number indicates the engine power (according to 1955 standards). The third number differentiates between brakes and transmission (chain drive or Cardan shafts). Small locomotives of the former Ka series were given the new class numbers 381 (pre-war models) and 382 (new models). The existing [[narrow gauge railway|narrow gauge]] locomotives of the [[Wangerooge Island Railway]] became Class 329. In 1987 the [[DB Class V 60|DB Class&amp;amp;nbsp;260/261]] were also assigned to the small locomotives and labelled as Class 360/361.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[History of rail transport in Germany]]&lt;br /&gt;
*[[Deutsche Bundesbahn]]&lt;br /&gt;
*[[UIC classification]]&lt;br /&gt;
&lt;br /&gt;
{{German locomotives}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Db Locomotive Classification}}&lt;br /&gt;
[[Category:Locomotives of Germany]]&lt;br /&gt;
[[Category:Locomotive classification systems]]&lt;/div&gt;</summary>
		<author><name>131.111.185.88</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Catenoid&amp;diff=3558</id>
		<title>Catenoid</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Catenoid&amp;diff=3558"/>
		<updated>2013-03-12T08:38:57Z</updated>

		<summary type="html">&lt;p&gt;131.111.16.20: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{one source|date=December 2009}}&lt;br /&gt;
[[File:Paraboloid of Revolution.svg|thumb|Axially symmetrical paraboloid. The inside surface is concave]]&lt;br /&gt;
&lt;br /&gt;
A &#039;&#039;&#039;rotating furnace&#039;&#039;&#039; is a device for making solid objects which have concave surfaces that are segments of [[Axial symmetry|axially symmetrical]] [[paraboloid]]s. Usually, the objects are made of [[glass]]. The [[furnace]] makes use of the fact, which was known already to [[Isaac Newton|Newton]], that the centrifugal-force-induced shape of the top surface of a spinning liquid is a concave paraboloid, identical to the shape of a reflecting telescope&#039;s primary focusing mirror.&lt;br /&gt;
&lt;br /&gt;
They can be used in various ways, including (after being [[silvered]]) as [[primary mirror]]s in [[reflecting telescope]]s; they have also been used for [[solar cooker]]s.&amp;lt;ref&amp;gt;http://solarcooking.org/research/SpinningParaboicConcentrators.htm&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Design ==&lt;br /&gt;
[[File:Coriolis effect11.jpg|thumb|Parabolic shape formed by a liquid surface under rotation. Two liquids of different densities completely fill a narrow space between two sheets of plexiglass. The gap between the sheets is closed at the bottom, sides and top. The whole assembly is rotating around a vertical axis passing through the centre]]&lt;br /&gt;
&lt;br /&gt;
The furnace includes a mechanism that rotates an open-topped container at constant speed around a vertical axis. A quantity of glass sufficient to make the mirror is placed in the container, heated until it is completely molten, and then allowed to cool while continuing to rotate until it has completely solidified. When the rotation is stopped, the glass is solid, so the paraboloidal shape of its top surface is preserved. This process is called &#039;&#039;spin casting&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
The same process can be used to make a [[lens (optics)|lens]] with a concave paraboloidal surface. The other surface is shaped by the container that holds the molten glass acting as a mould. Lenses made this way are sometimes used as [[Objective (optics)|objectives]] in [[refracting telescope]]s.&lt;br /&gt;
&lt;br /&gt;
The word &#039;&#039;spin&#039;&#039; is frequently used in this context without implying that the rotation is rapid. Making a mirror with a focal length of five metres, for example, requires a rotation speed less than ten revolutions per minute. Since the speed is low, accurate [[Balancing of rotating masses|dynamic balancing]] of the rotating components is not needed.&lt;br /&gt;
&lt;br /&gt;
The axis of rotation becomes the axis of the paraboloid. It is not necessary for this axis to be in the centre of the container of glass, or even for it to pass through the container. By placing the container away from the axis, off-axis paraboloidal segments can be cast. This is done in the making of very large telescopes which have mirrors consisting of several segments.&lt;br /&gt;
&lt;br /&gt;
== Mathematical model ==&lt;br /&gt;
[[File:Forces in a Parabolic Dish.svg|thumb|The force of gravity (red), the [[normal force]] (green), and the resultant centripetal force (blue)]]&lt;br /&gt;
&lt;br /&gt;
In fluid mechanics, the state when no part of the fluid has motion relative to any other part of the fluid is called &#039;solid body rotation&#039;. When the liquid has reached a state of solid body rotation, then the dynamic equilibrium can be understood as a balance of two energies: gravitational [[potential energy]], and [[rotational kinetic energy]]. When a fluid is in solid body rotation it is the lowest state of energy that is available, because in a state of solid body rotation there is no friction to [[dissipation|dissipate]] any of the energy.&lt;br /&gt;
&lt;br /&gt;
In an inertial reference frame, the dynamic equilibrium cannot be understood in terms of an equilibrium of forces. This is because when the liquid is rotating, there is an unbalanced force acting on the liquid – the force of gravity is acting in a vertical direction on the liquid, and the surface of the parabolic dish exerts a [[normal force]] on the liquid resting on it. The resultant force is a net centripetal force toward the axis of rotation.&lt;br /&gt;
&lt;br /&gt;
The kinetic energy of a parcel of liquid given by the formula: &amp;lt;math&amp;gt;E_{kin} = \frac{1}{2} m v^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In the case of circular motion the relation &amp;lt;math&amp;gt;v = \omega r&amp;lt;/math&amp;gt; holds (&amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt; is in radians per second), hence &amp;lt;math&amp;gt;E_{kin} = \frac{1}{2} m \omega^2 r^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The gravitational potential energy is given by &amp;lt;math&amp;gt;E_{pot} = m g h&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;g&amp;lt;/math&amp;gt; is the acceleration of gravity and &amp;lt;math&amp;gt;h&amp;lt;/math&amp;gt; is the height of the liquid&#039;s surface above some arbitrary elevation, for instance, we can set &amp;lt;math&amp;gt;h=0&amp;lt;/math&amp;gt; to be the lowest liquid surface. We set the potential energy equal to the kinetic energy to find the liquid&#039;s shape: &amp;lt;math&amp;gt;h = \frac{1}{2 g} \omega^2 r^2&amp;lt;/math&amp;gt; This is of the form &amp;lt;math&amp;gt;h=kr^2&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt; is a constant, which is, by definition, a [[paraboloid]].&lt;br /&gt;
&lt;br /&gt;
It is not necessary to invoke the equality of rotational kinetic energy and gravitational potential energy. With reference to the force diagram above, the vertical component of the normal force (green arrow) must equal the weight of the parcel (red arrow), which is &amp;lt;math&amp;gt;mg&amp;lt;/math&amp;gt;, and the horizontal component of the normal force must equal the [[centripetal force]] (blue arrow) that keeps the parcel in circular motion, which is &amp;lt;math&amp;gt;m \omega^2 r&amp;lt;/math&amp;gt;. Since the green arrow is perpendicular to the surface of the liquid, the slope of the surface must equal the quotient of these forces: &amp;lt;math&amp;gt;\frac{d h}{d r} = \frac{m \omega^2 r}{m g}&amp;lt;/math&amp;gt; Cancelling the &amp;lt;math&amp;gt;m&amp;lt;/math&amp;gt;&#039;s, integrating, and setting &amp;lt;math&amp;gt;h=0&amp;lt;/math&amp;gt; when &amp;lt;math&amp;gt;r=0&amp;lt;/math&amp;gt; leads to &amp;lt;math&amp;gt;h = \frac{1}{2 g} \omega^2 r^2&amp;lt;/math&amp;gt; which is identical to the result obtained by the previous method, and likewise shows that the liquid surface is paraboloidal.&lt;br /&gt;
&lt;br /&gt;
The focal length of the paraboloid is related to the angular speed at which the liquid is rotated by the equation: &amp;lt;math&amp;gt;2f \omega^2=g&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; is the focal length, &amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt; is the rotation speed, and &amp;lt;math&amp;gt;g&amp;lt;/math&amp;gt; is the [[Gravitational acceleration|acceleration due to gravity]]. They must be in compatible units so, for example, &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; can be in metres, &amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt; in radians per second, and &amp;lt;math&amp;gt;g&amp;lt;/math&amp;gt; in metres per second-squared. The angle unit in &amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt; must be [[radian]]s. 1 radian per second is about 9.55 rotations per minute ([[RPM]]). On the Earth&#039;s surface, &amp;lt;math&amp;gt;g&amp;lt;/math&amp;gt; is about 9.81 metres per second-squared. Putting these numbers into the equation produces the approximation: &amp;lt;math&amp;gt;fs^2 \approx 447&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; is the focal length in metres, and &amp;lt;math&amp;gt;s&amp;lt;/math&amp;gt; is the rotation speed in RPM.&lt;br /&gt;
&lt;br /&gt;
== Uses ==&lt;br /&gt;
&lt;br /&gt;
Generally, a spin-cast paraboloid is not sufficiently accurate to permit its immediate use as a telescope mirror or lens, so it is corrected by computer-controlled grinding machines. The amount of grinding done, and the mass of glass material wasted, are much less than would have been required without spinning.&lt;br /&gt;
&lt;br /&gt;
Spin casting can also be used, often with materials other than glass, to produce prototype paraboloids, such as spotlight reflectors or solar-energy concentrators, which do not need to be as exactly paraboloidal as telescope mirrors. Spin casting every paraboloid that is made would be too slow and costly, so the prototype is simply copied relatively quickly and cheaply and with adequate accuracy.&lt;br /&gt;
&lt;br /&gt;
[[Liquid mirror telescope]]s have rotating mirrors that consist of a liquid metal such as [[mercury (element)|mercury]] or a [[low-melting alloy]] of [[gallium]]. The mirrors do not solidify, but are used while liquid and rotating. The rotation shapes them into paraboloids that are accurate enough to be used as primary reflectors in telescopes. No correction of the shape is necessary. Spin-cast glass mirrors need correction because of distortions that arise during and after solidification.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
* [[List of largest optical reflecting telescopes]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Telescopes]]&lt;br /&gt;
[[Category:Optics]]&lt;/div&gt;</summary>
		<author><name>131.111.16.20</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=P-y_method&amp;diff=12599</id>
		<title>P-y method</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=P-y_method&amp;diff=12599"/>
		<updated>2012-12-25T22:02:48Z</updated>

		<summary type="html">&lt;p&gt;131.111.250.181: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[combinatorics]], &#039;&#039;&#039;block walking&#039;&#039;&#039; is a method useful in thinking about sums of combinations graphically as &amp;quot;walks&amp;quot; on [[Pascal&#039;s triangle]]. As the name suggests, block walking problems involve counting the number of ways an individual can walk from one corner A of a city block to another corner B of another city block given restrictions on the number of blocks the person may walk, the directions the person may travel, the distance from A to B, et cetera.&lt;br /&gt;
&lt;br /&gt;
==An Example Block Walking Problem==&lt;br /&gt;
&lt;br /&gt;
Suppose such an individual, say &amp;quot;Fred&amp;quot;, must walk exactly k blocks to get to a point B that is exactly k blocks from A. It is convenient to regard Fred&#039;s starting point A as the [[Origin (mathematics)|origin]], &amp;lt;math&amp;gt;(0,0)&amp;lt;/math&amp;gt;, of a [[lattice (group)|rectangular array]] of [[lattice points]] and B as some lattice point &amp;lt;math&amp;gt;(e,n)&amp;lt;/math&amp;gt;, e units &amp;quot;East&amp;quot; and n units &amp;quot;North&amp;quot; of A, where &amp;lt;math&amp;gt;e+n=k&amp;lt;/math&amp;gt; and both &amp;lt;math&amp;gt;e&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; are nonnegative.&lt;br /&gt;
&lt;br /&gt;
===Solution by Brute Force===&lt;br /&gt;
A [[brute force (mathematics)|&amp;quot;brute force&amp;quot;]] solution to this problem may be obtained by systematically counting the number of ways Fred can reach each point &amp;lt;math&amp;gt;X=(x_1,x_2)&amp;lt;/math&amp;gt; where&lt;br /&gt;
:&amp;lt;math&amp;gt;0 \le x_{1} \le e&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;0 \le x_{2} \le n&amp;lt;/math&amp;gt;&lt;br /&gt;
without backtracking (i.e. only traveling North or East from one point to another) until a pattern is observed. For example, the number of ways Fred could go from &amp;lt;math&amp;gt;(0,0)&amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;(1,0)&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;(0,1)&amp;lt;/math&amp;gt; is exactly one;  to &amp;lt;math&amp;gt;(1,1)&amp;lt;/math&amp;gt; is two; to &amp;lt;math&amp;gt;(2,0)&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;(0,2)&amp;lt;/math&amp;gt; is one; to &amp;lt;math&amp;gt;(1,2)&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;(2,1)&amp;lt;/math&amp;gt; is three; and so on. Actually, you could receive the number of ways to get to a particular point by adding up the number of ways you can get to the point south of it and the number of ways you can get to the point west of it.(With the starting point being zero and all the points directly north and south of it one. ) In general, one soon discovers that the number of paths from A to any such X corresponds to an entry of [[Pascal&#039;s Triangle]].&lt;br /&gt;
&lt;br /&gt;
===Combinatorial Solution===&lt;br /&gt;
Since the problem involves counting a finite, discrete number of paths between lattice points, it is reasonable to assume a [[Combinatorial proof|combinatorial solution]] exists to the problem. Towards this end, we note that for Fred to still be on a path that will take him from A to B over &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt; blocks, at any point X he must either travel along one of the unit vectors &amp;lt;1,0&amp;gt; and &amp;lt;0,1&amp;gt;. For the sake of clarity, let &amp;lt;math&amp;gt;E=&amp;lt;1,0&amp;gt;&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;N=&amp;lt;0,1&amp;gt;&amp;lt;/math&amp;gt;. Given the coordinates of B, regardless of the path Fred travels he must walk along the vectors E and N exactly &amp;lt;math&amp;gt;e&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; times, respectively. As such, the problem reduces to finding the number of distinct rearrangements of the word&lt;br /&gt;
:&amp;lt;math&amp;gt; \overbrace{ EE \cdots E }^{e\text{ times}}\underbrace{ NN \cdots N }_{n \text{ times}}&amp;lt;/math&amp;gt;,&lt;br /&gt;
which is equivalent to finding the number of ways to choose &amp;lt;math&amp;gt;e&amp;lt;/math&amp;gt; indistinct objects from a group of &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt;. Thus the total number of paths Fred could take from A to B traveling only &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt; blocks is&lt;br /&gt;
:&amp;lt;math&amp;gt;\binom{k}{e}=\binom{k}{n}=\frac{k!}{e! n!}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Other Problems with Known, Block Walking Combinatorial Proofs==&lt;br /&gt;
* Proving that&lt;br /&gt;
:&amp;lt;math&amp;gt; \sum_{k=0}^n { n \choose k}^2\ = { 2n \choose n} &amp;lt;/math&amp;gt;&lt;br /&gt;
can be done with a straightforward application of block walking.&amp;lt;ref&amp;gt;Lehoczky, Sandor and Richard Rusczyk. &#039;&#039;The Art of Problem Solving, Volume II&#039;&#039;. Page 231.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
[[Category:Combinatorics]]&lt;/div&gt;</summary>
		<author><name>131.111.250.181</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Continuous-time_Markov_process&amp;diff=236478</id>
		<title>Continuous-time Markov process</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Continuous-time_Markov_process&amp;diff=236478"/>
		<updated>2012-06-05T20:05:34Z</updated>

		<summary type="html">&lt;p&gt;131.111.184.100: /* Embedded Markov chain */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== the body is very important ==&lt;br /&gt;
&lt;br /&gt;
Infants. Just the internal organs, your body has クリスチャンルブタン 激安 to die. &#039;Blood acoustic Pei Qin Yu sounded in mind for comprehension, the body is very important, once the body has been destroyed. Sanxian that only practice.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&#039;Really?&#039;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Qin Yu Pei put a backhand grab a blood Yuan Ying caught in his hand.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&#039;You ......&#039; Pei blood Qin Yu Yuan Ying looked incredible wounds クリスチャンルブタン アウトレット have クリスチャンルブタンジャパン disappeared without a trace in the chest. Just also stabbed a fist-sized wound. Such a big injury, plus internal organs injured. Logically Qin Yu&#039;s body has been finished, but ......&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Qin Yu クリスチャンルブタン 日本 did not waste time, directly underlying strength startled, Pei blood soul shattered, followed by a ring of black income Yuan Ying Yan Jun.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;say a long time.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;actually blood from Pei attack, to Bae blood killed. Time is only a breath, a master war. Although クリスチャンルブタン 東京 the fight several times during the attack, but in fact it is extremely time consuming short.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;by gravity field of rational use, and powerful body&lt;br /&gt;
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== sixteenth set of sixty-second chapter dowry ==&lt;br /&gt;
&lt;br /&gt;
Fang Wang, who is also a moment to God.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;that sat on クリスチャンルブタン 店舗 the edge of the week was also stunned.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;not a first-class obscurity Lingbao! Lingbao is second-rate top-level obscurity to weapons only.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Jiang Vatican stunned for a moment to react. クリスチャンルブタン 取扱店 Smile still on his face immediately:. &#039;This whip is second-rate Lingbao obscurity to the top weapon in grace?.&#039; Jiang Fan look like a pair of satisfaction.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Qin Yu smiled. Soon will step down.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;week was abstaining in time. Qin Yu will have a decision. Do not need to come up with first-class obscurity Lingbao, this second-rate to peak in obscurity Lingbao weapons. クリスチャンルブタン 店舗 Sufficient to obtain a third places.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;After all, other people have abstained, and the remaining two Quinn Hou and Shentu Where, Is able to クリスチャンルブタン 銀座 come up with a first-class obscurity Lingbao? if they クリスチャンルブタン do have second-tier obscurity Lingbao not necessarily even get results, the estimated support Qin Yu Carpenter this earth god, the king is certainly up to it.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;sixteenth set of sixty-second chapter dowry&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&#039;next.&#039; Jiang Fan cool and the sound echoed in the hall&lt;br /&gt;
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== But said self-comforting ==&lt;br /&gt;
&lt;br /&gt;
But said self-comforting, create exercises success, not to talk about it as a.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&#039;Puchi!&#039;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;black wind will be a knife to cut off a large piece of meat shoulders.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&#039;Well, concentrate on their way.&#039; Qin Yu rushed acoustic road.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;three brothers never talk too much, but quietly [http://www.lamartcorp.com/modules/mod_menu/rakuten_cl_1.php クリスチャンルブタン 価格] hurry, just three brothers did not help flying side by side, the trio enjoying the three brothers in the mortal world, with the last period of [http://www.lamartcorp.com/modules/mod_menu/rakuten_cl_5.php クリスチャンルブタン ブーツ] time.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;an elegant dodge, an avoidance.&amp;lt;br&amp;gt;between&amp;lt;br&amp;gt;brothers occasionally a smile, or a knife after being hurt wind humorous expression.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;......&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;into [http://www.lamartcorp.com/modules/mod_menu/rakuten_cl_12.php クリスチャンルブタン 値段] the [http://www.lamartcorp.com/modules/mod_menu/rakuten_cl_3.php クリスチャンルブタン 靴] last one hundred million years or so away, has been close to three years, and stands to reason that everyone should arrive abyss of death, but they have not yet seen the [http://www.lamartcorp.com/modules/mod_menu/rakuten_cl_6.php クリスチャンルブタン 中古] abyss of death, we can only move forward!&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;but the situation on the road shows here from the abyss of death must close.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;because more and more intensive air knife,&lt;br /&gt;
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		<author><name>131.111.184.100</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Discontinuous_linear_map&amp;diff=245660</id>
		<title>Discontinuous linear map</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Discontinuous_linear_map&amp;diff=245660"/>
		<updated>2012-06-03T11:47:53Z</updated>

		<summary type="html">&lt;p&gt;131.111.220.6: /* concrete example */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The author&#039;s name is Christy. Mississippi is exactly where his home is. To play lacross is the thing I love most of all. He is an order clerk and it&#039;s something he truly appreciate.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;My blog post - psychic chat online, [http://galab-work.cs.pusan.ac.kr/Sol09B/?document_srl=1489804 pusan.ac.kr],&lt;/div&gt;</summary>
		<author><name>131.111.220.6</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Bartlett%27s_test&amp;diff=241754</id>
		<title>Bartlett&#039;s test</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Bartlett%27s_test&amp;diff=241754"/>
		<updated>2012-05-28T17:20:25Z</updated>

		<summary type="html">&lt;p&gt;131.111.111.93: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== A similar Vibram Kso Womens ==&lt;br /&gt;
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		<author><name>131.111.111.93</name></author>
	</entry>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Kruskal%E2%80%93Katona_theorem&amp;diff=238780</id>
		<title>Kruskal–Katona theorem</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Kruskal%E2%80%93Katona_theorem&amp;diff=238780"/>
		<updated>2012-05-17T14:59:06Z</updated>

		<summary type="html">&lt;p&gt;131.111.184.8: /* Statement for uniform hypergraphs */   removed false statement&lt;/p&gt;
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== Ray Ban Brillen  ist Ihr Budget. ==&lt;br /&gt;
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