2005
DOI: 10.1103/physrevb.72.144524
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Integrable dynamics of coupled Fermi-Bose condensates

Abstract: We study the mean-field dynamics of a fermionic condensate interacting with a single bosonic mode (a generalized Dicke model). This problem is integrable and can be mapped onto a corresponding BCS problem. We derive the general solution and a full set of integrals of motion for the time evolution of coupled Fermi-Bose condensates. The present paper complements our earlier study of the dynamics of the BCS model (cond-mat/0407501 and cond-mat/0505493). Here we provide a self-contained introduction to the variabl… Show more

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Cited by 57 publications
(96 citation statements)
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“…In the case g i = g the model we have considered is exactly solvable, and its solution is equivalent to that of the BCS model [36]. The linear stability analysis above can be extended by linking it to the exact solutions through the concept of the Lax vector.…”
Section: Exact Solutionsmentioning
confidence: 99%
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“…In the case g i = g the model we have considered is exactly solvable, and its solution is equivalent to that of the BCS model [36]. The linear stability analysis above can be extended by linking it to the exact solutions through the concept of the Lax vector.…”
Section: Exact Solutionsmentioning
confidence: 99%
“…The next simplest solutions correspond to an ansatz proposed by Barankov and Levitov [38], and have oscillations of the order parameter described by elliptic functions. An approach for determining the type of solution which evolves from a given initial condition is discussed in [39], and can be applied to the Dicke model using the Lax vector given in [36].…”
Section: Exact Solutionsmentioning
confidence: 99%
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“…The Lax vector L(w) is a three-dimensional vector whose components are rational polynomials of an auxiliary complex variable w and is defined as [43] …”
Section: Analysis Of the Pairing Oscillationsmentioning
confidence: 99%
“…Time-dependent couplings can be realized, for example, by varying the intensity of the laser that fixes the amplitude of an optical lattice or by changing the atomic scattering length through sweeping an external magnetic field across a Feshbach resonance. This problem, which has attracted a lot of attention recently [4,5,6,7,8,9,10,11,12,13,14,15,16,17,18], is what we consider as well.…”
Section: Introductionmentioning
confidence: 99%