2015
DOI: 10.1088/1742-6596/597/1/012025
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The Dicke model as the contraction limit of a pseudo-deformed Richardson-Gaudin model

Abstract: The Dicke model is derived in the contraction limit of a pseudo-deformation of the quasispin algebra in the su(2)-based Richardson-Gaudin models. Likewise, the integrability of the Dicke model is established by constructing the full set of conserved charges, the form of the Bethe Ansatz state, and the associated Richardson-Gaudin equations. Thanks to the formulation in terms of the pseudo-deformation, the connection from the su(2)-based Richardson-Gaudin model towards the Dicke model can be performed adiabatic… Show more

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Cited by 5 publications
(6 citation statements)
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References 276 publications
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“…In this context, exact Bethe ansatz solvable models have been particularly fruitful to the study of quantum dynamics of this kind, for example, integrability-based central spin problems [28][29][30][31][32][33][34][35][36][37][38][39], atom-field interacting systems in quantum nonlinear optics [4,40,41], thermalization and quantum dynamics [42][43][44][45], and quantum hydrodynamics [46,47], etc. However, the problem of the size of the Hilbert space increasing exponentially with the particle number still prohibits full analytical accesses to the quantum dynamics at a many-body level.…”
mentioning
confidence: 99%
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“…In this context, exact Bethe ansatz solvable models have been particularly fruitful to the study of quantum dynamics of this kind, for example, integrability-based central spin problems [28][29][30][31][32][33][34][35][36][37][38][39], atom-field interacting systems in quantum nonlinear optics [4,40,41], thermalization and quantum dynamics [42][43][44][45], and quantum hydrodynamics [46,47], etc. However, the problem of the size of the Hilbert space increasing exponentially with the particle number still prohibits full analytical accesses to the quantum dynamics at a many-body level.…”
mentioning
confidence: 99%
“…A j (s x 0 s x j + s y 0 s y j ) + ∆ j s z 0 s z j , (1) where B is an effective external magnetic field for the central spin [53], N is the number of spins in the bath, A j is the transverse coupling amplitude, and ∆ j is the longitudinal interaction. The model ( 1) is integrable if ∆ j and A j are related through ∆ 2 j −A 2 j = Const., see [32,38,39]. Although this type of models, e.g.…”
mentioning
confidence: 99%
“…The model is integrable for the coupling constant A k and ∆ k with a constraint. [10][11][12][13][14][15] For the θ = 0 case, the eigenvalues and eigenstates of the Hamiltonian (1) can be exactly solved by the algebraic Bethe ansatz method. [16,17] Based on the exact solutions, on the one hand, an efficient technique has been devised for the numerical solution of the Bethe ansatz equations (BAEs); [18] on the other hand, the thermodynamic limit of the models is a subject of intense research.…”
Section: Introductionmentioning
confidence: 99%
“…( 3) can be derived from the Gaudin algebra (see, for example, Refs. [9,11,37,38]). Note that there also exists a class of spin-1/2 XXZ integrable models built from non-skew symmetric r-matrices, which do not necessarily obey Eq.…”
Section: Introductionmentioning
confidence: 99%