2009
DOI: 10.1103/physreva.80.023810
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Large-Nscaling behavior of the ground-state energy, fidelity, and the order parameter in the Dicke model

Abstract: Within the numerically exact solution to the Dicke model proposed previously, we study the quantum criticality in terms of the ground-state (GS) energy, fidelity, and the order parameter.The finite size scaling analysis for the average fidelity susceptibility (FS) and second derivative of GS energy are performed. The correlation length exponent is obtained to be ν = 2/3, which is the same as that in Lipkin-Meshkov-Glick model obtained previously, suggesting the same universality.It is observed that average FS … Show more

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Cited by 70 publications
(20 citation statements)
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“…9(c) we show the scaling of the QFI with N (16) which is characterized by an exponent γ = 2/3. The same scaling has been provided for the the QFI (or equivalently fidelity susceptibility) in the Lipkin-Meshkow-Glick [44], Dicke [45] and bosonic Josephson junction [8] models [55]. Consequently, it suggests that the antiferromagnetic spinor condensate hosts a second-order quantum phase transition in the same universal class of these systems.…”
Section: Discussionmentioning
confidence: 58%
“…9(c) we show the scaling of the QFI with N (16) which is characterized by an exponent γ = 2/3. The same scaling has been provided for the the QFI (or equivalently fidelity susceptibility) in the Lipkin-Meshkow-Glick [44], Dicke [45] and bosonic Josephson junction [8] models [55]. Consequently, it suggests that the antiferromagnetic spinor condensate hosts a second-order quantum phase transition in the same universal class of these systems.…”
Section: Discussionmentioning
confidence: 58%
“…In the realm of traditional quantum mechanics, the geometric phase has been introduced to analyze the quantum phase transitions of the XY model [15][16][17] and much effort has been devoted to various Hermitian many-body systems [18][19][20][21][22][23][24][25][26].…”
Section: Introductionmentioning
confidence: 99%
“…In fact, the Dicke model with j ≥ 1 for nonzero energy splitting between the two levels of the single atom is formally not integrable when λ/ω 0 → ∞, though the model is exactly solvable and integrable when j = 1/2, as recently pointed out by Braak [16,20]. Braak's exact solution to the Dicke model with j = 1/2 was also recovered [50,51] by using the Bogoliubov operators and the method proposed in [22], respectively, while the finite size Dicke model was also studied within the shifted boson basis in [52], which confirms Braak's observations on the exact solvability of the Dicke model, though the model is not integrable in general. However, the Poissonian limit is reached as λ/ω 0 → ∞ at the resonance point, which is also demonstrated in [10].…”
Section: Level Statistical Propertiesmentioning
confidence: 85%
“…As a remedy, instead of the Dicke basis, the Dicke Hamiltonian can be diagonalized in a shifted boson basis where convergence is reached with a smaller number of shifted boson states across the whole coupling regime [21]. This approach was also used to study the quantum criticality, the finite size effects, fidelity and the order parameter in the Dicke model [22].…”
Section: Introductionmentioning
confidence: 99%