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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]]. | |||
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
and its adjoint
Their commutation relation is
where is the vacuum state of the harmonic oscillator.
They may be regarded as a (exponential of) phase operator because
where is the number operator. So the exponential of the phase operator displaces the number operator in the same fashion as .
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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- ↑ L. Susskind and J. Glogower, Physica 1, 49 (1964)
- ↑ 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.
- ↑ 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
- ↑ 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