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The '''Susskind-Glogower operator''', first proposed by [[Leonard Susskind]] and J. Glogower,<ref>L. Susskind and J. Glogower, Physica 1, 49 (1964)</ref> refers to the operator where the phase is introduced as an approximate polar decomposition of the [[creation and annihilation operators]].


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It is defined as
 
: <math> V=\frac{1}{\sqrt{aa^{\dagger}}}a</math>,
and its adjoint
: <math> V^{\dagger}=a^{\dagger}\frac{1}{\sqrt{aa^{\dagger}}}</math>.
 
Their [[commutation relation]] is
 
: <math> [V,V^{\dagger}]=|0\rangle\langle 0|</math>,
 
where  <math> |0\rangle</math> is the vacuum state of the [[harmonic oscillator]].
 
They may be regarded as a (exponential of) [[phase operator]] because
 
: <math>Va^{\dagger}a V^{\dagger}=a^{\dagger}a+1</math>,
 
where <math>a^{\dagger}a</math> is the number operator. So the exponential of the phase operator displaces the [[number operator]] in the same fashion as
<math>\exp\left(i\frac{px_o}{\hbar}\right)x\exp\left(-i\frac{px_o}{\hbar}\right)=x+x_0</math>.
 
They may be used to solve problems such as atom-field interactions,<ref>B. M. Rodríguez-Lara and H.M. Moya-Cessa,
Journal of Physics A 46, 095301 (2013). Exact solution of generalized Dicke models via Susskind-Glogower operators
http://dx.doi.org/10.1088/1751-8113/46/9/095301.</ref> level-crossings  <ref>B.M. Rodríguez-Lara, D. Rodríguez-Méndez and H. Moya-Cessa, Physics Letters A 375, 3770-3774 (2011). Solution to the Landau-Zener problem via Susskind-Glogower operators.
http://dx.doi.org/10.1016/j.physleta.2011.08.051</ref> or to define some class of [[non-linear coherent states]],<ref>R. de J. León-Montiel, H. Moya-Cessa, F. Soto-Eguibar,
Revista Mexicana de Física S 57, 133 (2011). Nonlinear coherent states for the Susskind-Glogower operators.
http://rmf.smf.mx/pdf/rmf-s/57/3/57_3_133.pdf</ref> among others.
 
==References==
{{reflist}}
 
{{DEFAULTSORT:Susskind-Glogower Operator}}
[[Category:Quantum mechanics]]

Revision as of 12:14, 20 March 2013

The Susskind-Glogower operator, first proposed by Leonard Susskind and J. Glogower,[1] refers to the operator where the phase is introduced as an approximate polar decomposition of the creation and annihilation operators.

It is defined as

V=1aaa,

and its adjoint

V=a1aa.

Their commutation relation is

[V,V]=|00|,

where |0 is the vacuum state of the harmonic oscillator.

They may be regarded as a (exponential of) phase operator because

VaaV=aa+1,

where aa is the number operator. So the exponential of the phase operator displaces the number operator in the same fashion as exp(ipxo)xexp(ipxo)=x+x0.

They may be used to solve problems such as atom-field interactions,[2] level-crossings [3] or to define some class of non-linear coherent states,[4] among others.

References

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  1. L. Susskind and J. Glogower, Physica 1, 49 (1964)
  2. B. M. Rodríguez-Lara and H.M. Moya-Cessa, Journal of Physics A 46, 095301 (2013). Exact solution of generalized Dicke models via Susskind-Glogower operators http://dx.doi.org/10.1088/1751-8113/46/9/095301.
  3. B.M. Rodríguez-Lara, D. Rodríguez-Méndez and H. Moya-Cessa, Physics Letters A 375, 3770-3774 (2011). Solution to the Landau-Zener problem via Susskind-Glogower operators. http://dx.doi.org/10.1016/j.physleta.2011.08.051
  4. R. de J. León-Montiel, H. Moya-Cessa, F. Soto-Eguibar, Revista Mexicana de Física S 57, 133 (2011). Nonlinear coherent states for the Susskind-Glogower operators. http://rmf.smf.mx/pdf/rmf-s/57/3/57_3_133.pdf