2004
DOI: 10.1103/physrevb.69.054403
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Crossover from Poisson to Wigner-Dyson level statistics in spin chains with integrability breaking

Abstract: We study numerically the evolution of energy-level statistics as an integrability-breaking term is added to the XXZ Hamiltonian. For finite-length chains, physical properties exhibit a crossover from behavior resulting from the Poisson level statistics characteristic of integrable models to behavior corresponding to the Wigner-Dyson statistics characteristic of the random-matrix theory used to describe chaotic systems. Different measures of the level statistics are observed to follow different crossover patter… Show more

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Cited by 85 publications
(101 citation statements)
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“…However, we shall show that it is practically effective for finite-size quantum systems. In fact, the above conjecture has been numerically confirmed for many quantum spin systems such as correlated spin systems [1][2][3][4][5][6][7] and disordered spin systems. [8][9][10][11][12] In the Anderson model of disordered systems, P Poi (s) and P Wig (s) characterize the localized and the metallic phases, respectively.…”
Section: Introductionmentioning
confidence: 72%
“…However, we shall show that it is practically effective for finite-size quantum systems. In fact, the above conjecture has been numerically confirmed for many quantum spin systems such as correlated spin systems [1][2][3][4][5][6][7] and disordered spin systems. [8][9][10][11][12] In the Anderson model of disordered systems, P Poi (s) and P Wig (s) characterize the localized and the metallic phases, respectively.…”
Section: Introductionmentioning
confidence: 72%
“…Thus, an accurate characterization of its integrability properties in physical regimes of interest has both a fundamental and practical significance. In the special case of spin-1/2 particles, a partial characterization of the integrability-to-chaos transition has been achieved, based on both clean systems where chaos is induced by coupling two different spin chains [54] or by adding next-nearest-neighbor interactions [54,55,56], as well as disordered systems, where the integrabilitybreaking term consists of random magnetic fields applied to all or a subset of spins [57,58,59]. Aside from their relevance to model real materials, disordered systems offer the added advantage of providing a natural arena to study the interplay between interaction and disorder, which remains a most challenging problem in condensedmatter physics.…”
Section: Disordered Heisenberg Modelsmentioning
confidence: 99%
“…Poisson statistics have been numerically verified on a case-by-case basis for some quantum integrable systems, including the Hubbard [2] and Heisenberg [2,3] models. On the other hand, general or analytic results on the spectra of quantum integrable models are lacking, in part due to the absence of a generally accepted unambiguous notion of quantum integrability, [9,10] and in part because existing results usually apply to isolated models instead of members of statistical ensembles like random matrices [11].…”
Section: Introductionmentioning
confidence: 99%
“…the system cannot be represented as a collection of decoupled harmonic oscillators. As integrability is destroyed by perturbing the Hamiltonian, the statistics are expected to cross over from Poisson to Wigner-Dyson at perturbation strengths as small as the inverse system size [3].…”
Section: Introductionmentioning
confidence: 99%
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