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{{Lie groups |Representation}} | |||
In [[mathematics]] and [[theoretical physics]], the idea of a '''representation of a [[Lie group]]''' plays an important role in the study of continuous [[symmetry]]. A great deal is known about such representations, a basic tool in their study being the use of the corresponding 'infinitesimal' [[representation of Lie algebras|representations of Lie algebras]]. The physics literature sometimes passes over the distinction between Lie group representations and Lie algebra representations. | |||
== Representations on a complex finite-dimensional vector space == | |||
Let us first discuss representations acting on finite-dimensional complex vector spaces. A [[group representation|representation]] of a [[Lie group]] ''G'' on a finite-dimensional complex [[vector space]] ''V'' is a smooth [[group homomorphism]] Ψ:''G''→Aut(''V'') from ''G'' to the [[automorphism group]] of ''V''. | |||
For ''n''-dimensional ''V'', the automorphism group of ''V'' is identified with a subset of complex square-matrices of order ''n''. The automorphism group of ''V'' is given the structure of a smooth manifold using this identification. The condition that Ψ is smooth, in the definition above, means that Ψ is a smooth map from the smooth manifold ''G'' to the smooth manifold Aut(''V''). | |||
If a basis for the complex vector space ''V'' is chosen, the representation can be expressed as a homomorphism into [[general linear group|GL(''n'','''C''')]]. This is known as a ''matrix representation''. | |||
== Representations on a finite-dimensional vector space over an arbitrary field == | |||
A [[group representation|representation]] of a [[Lie group]] ''G'' on a [[vector space]] ''V'' (over a [[field (mathematics)|field]] ''K'') is a [[smooth function|smooth]] (i.e. respecting the differential structure) [[group homomorphism]] ''G''→Aut(''V'') from ''G'' to the [[automorphism group]] of ''V''. If a basis for the vector space ''V'' is chosen, the representation can be expressed as a homomorphism into [[general linear group|GL(''n'',''K'')]]. This is known as a ''matrix representation''. | |||
Two representations of ''G'' on vector spaces ''V'', ''W'' are ''equivalent'' if they have the | |||
same matrix representations with respect to some choices of bases | |||
for ''V'' and ''W''. | |||
On the Lie algebra level, there is a corresponding linear mapping from the Lie algebra of G to [[endomorphism|End(''V'')]] preserving the [[Lie_algebra#Definition_and_first_properties|Lie bracket]] [ , ]. See [[representation of Lie algebras]] for the Lie algebra theory. | |||
If the homomorphism is in fact a [[monomorphism]], the representation is said to be ''faithful''. | |||
A [[unitary representation]] is defined in the same way, except that G maps to [[unitary matrix|unitary matrices]]; the Lie algebra will then map to [[skew-hermitian]] matrices. | |||
If ''G'' is a compact Lie group, every finite-dimensional representation is equivalent to | |||
a unitary one. | |||
== Representations on Hilbert spaces == | |||
A [[group representation|representation]] of a [[Lie group]] ''G'' on a complex [[Hilbert space]] ''V'' is a [[group homomorphism]] Ψ:''G'' → B(''V'') from ''G'' to B(''V''), the group of bounded linear operators of ''V'' which have a bounded inverse, such that the map ''G''×''V'' → ''V'' given by (''g'',''v'') → Ψ(''g'')''v'' is continuous. | |||
This definition can handle representations on '''infinite-dimensional''' Hilbert spaces. Such representations can be found in e.g. quantum mechanics, but also in Fourier analysis as shown in the following example. | |||
Let ''G''='''R''', and let the complex Hilbert space ''V'' be ''L''<sup>2</sup>('''R'''). We define the representation Ψ:'''R''' → B(''L''<sup>2</sup>('''R''')) by Ψ(''r''){''f''(''x'')} → ''f''(''r''<sup>-1</sup>''x''). | |||
See also [[Wigner's classification]] for representations of the [[Poincaré group]]. | |||
== Classification == | |||
If G is a [[Semisimple Lie group|semisimple]] group, its finite-dimensional representations can be decomposed as [[direct sum of representations|direct sums]] of [[irreducible representation]]s. The irreducibles are indexed by highest [[weight (representation theory)|weight]]; the allowable (''dominant'') highest weights satisfy a suitable positivity condition. In particular, there exists a set of ''fundamental weights'', indexed by the vertices of the [[Dynkin diagram]] of G, such that dominant weights are simply non-negative integer linear combinations of the fundamental weights. The characters of the irreducible representations are given by the [[Weyl character formula]]. | |||
If G is a commutative [[Lie group]], then its irreducible representations are simply the continuous [[Character (mathematics)|character]]s of G: see [[Pontryagin duality]] for this case. | |||
A quotient representation is a [[quotient module]] of the [[group ring]]. | |||
== Formulaic examples == | |||
Let '''F'''<sub>''q''</sub> be a finite field of order ''q'' and characteristic ''p''. Let ''G'' be a finite group of Lie type, that is, ''G'' is the '''F'''<sub>''q''</sub>-rational points of a connected reductive group ''G'' defined over '''F'''<sub>''q''</sub>. For example, if ''n'' is a positive integer GL(''n'', '''F'''<sub>''q''</sub>) and SL(n, '''F'''<sub>''q''</sub>) are finite groups of Lie type. Let <math>J = \left [ \begin{smallmatrix}0 & I_n \\ -I_n & 0\end{smallmatrix} \right ]</math>, where ''I''<sub>n</sub> is the ''n''×''n'' identity matrix. Let | |||
: <math>Sp_2(\mathbb{F}_q) = \left \{ g \in GL_{2n}(\mathbb{F}_q) | ^tgJg = J \right \}.</math> | |||
Then Sp(2,'''F'''<sub>''q''</sub>) is a symplectic group of rank ''n'' and is a finite group of Lie type. For ''G'' = GL(''n'', '''F'''<sub>''q''</sub>) or SL(''n'', '''F'''<sub>''q''</sub>) (and some other examples), the ''[[standard Borel subgroup]]'' ''B'' of ''G'' is the subgroup of ''G'' consisting of the upper triangular elements in ''G''. A ''[[standard parabolic subgroup]]'' of ''G'' is a subgroup of ''G'' which contains the standard Borel subgroup ''B''. If ''P'' is a standard parabolic subgroup of GL(''n'', '''F'''<sub>''q''</sub>), then there exists a partition (''n''<sub>1</sub>, …, ''n''<sub>r</sub>) of ''n'' (a set of positive integers <math>n_j\,\!</math> such that <math>n_1 + \ldots + n_r = n\,\!</math>) such that <math>P = P_{(n_1,\ldots,n_r)} = M \times N</math>, where <math>M \simeq GL_{n_1}(\mathbb{F}_q) \times \ldots \times GL_{n_r}(\mathbb{F}_q)</math> has the form | |||
: <math>M = \left \{\left.\begin{pmatrix}A_1 & 0 & \cdots & 0 \\ 0 & A_2 & \cdots & 0 \\ \vdots & \ddots & \ddots & \vdots \\ 0 & \cdots & 0 & A_r\end{pmatrix}\right|A_j \in GL_{n_j}(\mathbb{F}_q), 1 \le j \le r \right \},</math> | |||
and | |||
: <math>N=\left \{\begin{pmatrix}I_{n_1} & * & \cdots & * \\ 0 & I_{n_2} & \cdots & * \\ \vdots & \ddots & \ddots & \vdots \\ 0 & \cdots & 0 & I_{n_r}\end{pmatrix}\right\},</math> | |||
where <math>*\,\!</math> denotes arbitrary entries in <math>\mathbb{F}_q</math>. | |||
<!--''This section is still in progress. It should be finished soon.''[[User:Vermin1302|Vermi]] 06:22, 26 October 2005 (UTC) --> | |||
==See also== | |||
*[[Representation theory of the Lorentz group]] | |||
*[[Representation theory of Hopf algebras]] | |||
*[[Adjoint representation of a Lie group]] | |||
*[[List of Lie group topics]] | |||
* [[Symmetry in quantum mechanics]] | |||
== References == | |||
* {{Fulton-Harris}} | |||
* {{Citation|first=Brian C.|last=Hall|title=Lie Groups, Lie Algebras, and Representations: An Elementary Introduction |publisher=Springer|year=2003|isbn=0-387-40122-9}}. | |||
* {{Citation|last=Knapp|first=Anthony W.|authorlink=Anthony Knapp|title=Lie Groups Beyond an Introduction|url=http://www.math.sunysb.edu/~aknapp/books/beyond2.html|edition= 2nd|series=Progress in Mathematics|volume=140|publisher=Birkhäuser|place= Boston|year= 2002}}. | |||
* {{Citation|last=Rossmann|first= Wulf |title=Lie Groups: An Introduction Through Linear Groups|series= Oxford Graduate Texts in Mathematics|publisher= Oxford University Press|isbn= 978-0-19-859683-7|year=2001}}. The 2003 reprint corrects several typographical mistakes. | |||
[[Category:Lie groups]] | |||
[[Category:Representation theory of Lie groups]] |
Revision as of 07:48, 24 October 2013
In mathematics and theoretical physics, the idea of a representation of a Lie group plays an important role in the study of continuous symmetry. A great deal is known about such representations, a basic tool in their study being the use of the corresponding 'infinitesimal' representations of Lie algebras. The physics literature sometimes passes over the distinction between Lie group representations and Lie algebra representations.
Representations on a complex finite-dimensional vector space
Let us first discuss representations acting on finite-dimensional complex vector spaces. A representation of a Lie group G on a finite-dimensional complex vector space V is a smooth group homomorphism Ψ:G→Aut(V) from G to the automorphism group of V.
For n-dimensional V, the automorphism group of V is identified with a subset of complex square-matrices of order n. The automorphism group of V is given the structure of a smooth manifold using this identification. The condition that Ψ is smooth, in the definition above, means that Ψ is a smooth map from the smooth manifold G to the smooth manifold Aut(V).
If a basis for the complex vector space V is chosen, the representation can be expressed as a homomorphism into GL(n,C). This is known as a matrix representation.
Representations on a finite-dimensional vector space over an arbitrary field
A representation of a Lie group G on a vector space V (over a field K) is a smooth (i.e. respecting the differential structure) group homomorphism G→Aut(V) from G to the automorphism group of V. If a basis for the vector space V is chosen, the representation can be expressed as a homomorphism into GL(n,K). This is known as a matrix representation. Two representations of G on vector spaces V, W are equivalent if they have the same matrix representations with respect to some choices of bases for V and W.
On the Lie algebra level, there is a corresponding linear mapping from the Lie algebra of G to End(V) preserving the Lie bracket [ , ]. See representation of Lie algebras for the Lie algebra theory.
If the homomorphism is in fact a monomorphism, the representation is said to be faithful.
A unitary representation is defined in the same way, except that G maps to unitary matrices; the Lie algebra will then map to skew-hermitian matrices.
If G is a compact Lie group, every finite-dimensional representation is equivalent to a unitary one.
Representations on Hilbert spaces
A representation of a Lie group G on a complex Hilbert space V is a group homomorphism Ψ:G → B(V) from G to B(V), the group of bounded linear operators of V which have a bounded inverse, such that the map G×V → V given by (g,v) → Ψ(g)v is continuous.
This definition can handle representations on infinite-dimensional Hilbert spaces. Such representations can be found in e.g. quantum mechanics, but also in Fourier analysis as shown in the following example.
Let G=R, and let the complex Hilbert space V be L2(R). We define the representation Ψ:R → B(L2(R)) by Ψ(r){f(x)} → f(r-1x).
See also Wigner's classification for representations of the Poincaré group.
Classification
If G is a semisimple group, its finite-dimensional representations can be decomposed as direct sums of irreducible representations. The irreducibles are indexed by highest weight; the allowable (dominant) highest weights satisfy a suitable positivity condition. In particular, there exists a set of fundamental weights, indexed by the vertices of the Dynkin diagram of G, such that dominant weights are simply non-negative integer linear combinations of the fundamental weights. The characters of the irreducible representations are given by the Weyl character formula.
If G is a commutative Lie group, then its irreducible representations are simply the continuous characters of G: see Pontryagin duality for this case.
A quotient representation is a quotient module of the group ring.
Formulaic examples
Let Fq be a finite field of order q and characteristic p. Let G be a finite group of Lie type, that is, G is the Fq-rational points of a connected reductive group G defined over Fq. For example, if n is a positive integer GL(n, Fq) and SL(n, Fq) are finite groups of Lie type. Let , where In is the n×n identity matrix. Let
Then Sp(2,Fq) is a symplectic group of rank n and is a finite group of Lie type. For G = GL(n, Fq) or SL(n, Fq) (and some other examples), the standard Borel subgroup B of G is the subgroup of G consisting of the upper triangular elements in G. A standard parabolic subgroup of G is a subgroup of G which contains the standard Borel subgroup B. If P is a standard parabolic subgroup of GL(n, Fq), then there exists a partition (n1, …, nr) of n (a set of positive integers such that ) such that , where has the form
and
where denotes arbitrary entries in .
See also
- Representation theory of the Lorentz group
- Representation theory of Hopf algebras
- Adjoint representation of a Lie group
- List of Lie group topics
- Symmetry in quantum mechanics
References
- Template:Fulton-Harris
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15.6.1 As the agent is an intermediary, generally, as soon as the principal and third party are introduced right into a contractual relationship, the agent drops out of the image, subject to any problems with remuneration or indemnification that he could have against the principal, and extra exceptionally, against the third occasion. Generally, agents are entitled to be indemnified for all liabilities reasonably incurred within the execution of the brokers´ authority.
To achieve the very best outcomes, you must be always updated on market situations, including past transaction information and reliable projections. You could review and examine comparable homes that are currently available in the market, especially these which have been sold or not bought up to now six months. You'll be able to see a pattern of such report by clicking here It's essential to defend yourself in opposition to unscrupulous patrons. They are often very skilled in using highly unethical and manipulative techniques to try and lure you into a lure. That you must also protect your self, your loved ones, and personal belongings as you'll be serving many strangers in your home. Sign a listing itemizing of all of the objects provided by the proprietor, together with their situation. HSR Prime Recruiter 2010. - Many property agents need to declare for the PIC grant in Singapore. However, not all of them know find out how to do the correct process for getting this PIC scheme from the IRAS. There are a number of steps that you need to do before your software can be approved.
Naturally, you will have to pay a safety deposit and that is usually one month rent for annually of the settlement. That is the place your good religion deposit will likely be taken into account and will kind part or all of your security deposit. Anticipate to have a proportionate amount deducted out of your deposit if something is discovered to be damaged if you move out. It's best to you'll want to test the inventory drawn up by the owner, which can detail all objects in the property and their condition. If you happen to fail to notice any harm not already mentioned within the inventory before transferring in, you danger having to pay for it yourself.
In case you are in search of an actual estate or Singapore property agent on-line, you simply should belief your intuition. It's because you do not know which agent is nice and which agent will not be. Carry out research on several brokers by looking out the internet. As soon as if you end up positive that a selected agent is dependable and reliable, you can choose to utilize his partnerise in finding you a home in Singapore. Most of the time, a property agent is taken into account to be good if he or she locations the contact data on his website. This may mean that the agent does not mind you calling them and asking them any questions relating to new properties in singapore in Singapore. After chatting with them you too can see them in their office after taking an appointment.
Have handed an trade examination i.e Widespread Examination for House Brokers (CEHA) or Actual Property Agency (REA) examination, or equal; Exclusive brokers are extra keen to share listing information thus making certain the widest doable coverage inside the real estate community via Multiple Listings and Networking. Accepting a severe provide is simpler since your agent is totally conscious of all advertising activity related with your property. This reduces your having to check with a number of agents for some other offers. Price control is easily achieved. Paint work in good restore-discuss with your Property Marketing consultant if main works are still to be done. Softening in residential property prices proceed, led by 2.8 per cent decline within the index for Remainder of Central Region
Once you place down the one per cent choice price to carry down a non-public property, it's important to accept its situation as it is whenever you move in – faulty air-con, choked rest room and all. Get round this by asking your agent to incorporate a ultimate inspection clause within the possibility-to-buy letter. HDB flat patrons routinely take pleasure in this security net. "There's a ultimate inspection of the property two days before the completion of all HDB transactions. If the air-con is defective, you can request the seller to repair it," says Kelvin.
15.6.1 As the agent is an intermediary, generally, as soon as the principal and third party are introduced right into a contractual relationship, the agent drops out of the image, subject to any problems with remuneration or indemnification that he could have against the principal, and extra exceptionally, against the third occasion. Generally, agents are entitled to be indemnified for all liabilities reasonably incurred within the execution of the brokers´ authority.
To achieve the very best outcomes, you must be always updated on market situations, including past transaction information and reliable projections. You could review and examine comparable homes that are currently available in the market, especially these which have been sold or not bought up to now six months. You'll be able to see a pattern of such report by clicking here It's essential to defend yourself in opposition to unscrupulous patrons. They are often very skilled in using highly unethical and manipulative techniques to try and lure you into a lure. That you must also protect your self, your loved ones, and personal belongings as you'll be serving many strangers in your home. Sign a listing itemizing of all of the objects provided by the proprietor, together with their situation. HSR Prime Recruiter 2010. The 2003 reprint corrects several typographical mistakes.