1991
DOI: 10.1007/bf01598977
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Quantum statistics of radiation in thermostat

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Cited by 10 publications
(12 citation statements)
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“…Eq. (26) is a Holstein-Primakoff [16] or Bogoliubov [17] transformation. When such a transformation exits, such as for the harmonic oscillator and for some other cases [23]- [25], there is no problem defining displacement-operator squeezed states.…”
Section: Squeezed Statesmentioning
confidence: 99%
“…Eq. (26) is a Holstein-Primakoff [16] or Bogoliubov [17] transformation. When such a transformation exits, such as for the harmonic oscillator and for some other cases [23]- [25], there is no problem defining displacement-operator squeezed states.…”
Section: Squeezed Statesmentioning
confidence: 99%
“…We consider an interaction between the particles and show that a lower energy state is obtained by taking into account fluctuations of the number of particles participating in the collective mode described by ϕ. For this purpose, we use the model considered by Bogoliubov [10]; we follow the derivation by Bogoliubov and reformulate it using the number changing operator and particle number conserving version of Bogoliubov operators. The Hamiltonian considered by Bogoliubov is given by…”
Section: Bogoliubov Operators Using the Number Changing Operators E ±Iθmentioning
confidence: 99%
“…This is the one adopted in the Gross-Pitaevskii theory [7,8]. This has to be supplemented by the condition for the absence of low energy excitations that will destroy the superfluidity; such a condition is given by Landau [9], and the excitation spectrum that satisfies it is provided by Bogoliubov [10], where the excitation spectrum was calculated using the particle number nonfixed formalism. Later, the same excitation spectrum was re-derived using the particle number fixed formalism by Leggett [6].…”
Section: Introductionmentioning
confidence: 99%
“…where each spin S i located at site i is a spin-5/2 with six discrete spin values, i.e., ±5/2, ±3/2 and ±1/2 and each spin σ j located at site j is a spin-7/2 that can take on eight discrete values ±7/2, ±5/2, ±3/2 and ±1/2. The most direct way of deriving the mean-field equations is to use the variational principle for the Gibbs free energy [32,33],…”
Section: The Model and The Mean-field Solutionmentioning
confidence: 99%