2011
DOI: 10.1088/1742-5468/2011/09/p09028
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The entanglement entropy of one-dimensional systems in continuous and homogeneous space

Abstract: Abstract.We introduce a systematic framework to calculate the bipartite entanglement entropy of a compact spatial subsystem in a one-dimensional quantum gas which can be mapped into a noninteracting fermion system. We show that when working with a finite number of particles N , the Rényi entanglement entropies grow as ln N , with a prefactor that is given by the central charge. We apply this novel technique to the ground state and to excited states of periodic systems. We also consider systems with boundaries.… Show more

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Cited by 83 publications
(139 citation statements)
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References 77 publications
(190 reference statements)
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“…[20] and elsewhere, there are also subleading oscillating terms in the Renyi entropy. Similar oscillations have been extensively studied in one dimension [25][26][27][28][29][30][31]. Here we compute these subleading oscillating terms in the Renyi entropy analytically for the free Fermi gas in higher dimensions.…”
Section: Introductionsupporting
confidence: 57%
“…[20] and elsewhere, there are also subleading oscillating terms in the Renyi entropy. Similar oscillations have been extensively studied in one dimension [25][26][27][28][29][30][31]. Here we compute these subleading oscillating terms in the Renyi entropy analytically for the free Fermi gas in higher dimensions.…”
Section: Introductionsupporting
confidence: 57%
“…If one is able to calculate (the asymptotic behaviour of) D A (λ), the entanglement entropies are given by Eq. (7) as the integral [75,79] …”
Section: Entanglement Entropies and Particle Fluctuationsmentioning
confidence: 99%
“…The possibility of turning these expansions into an effective measure of entanglement depends on its convergence properties, which appear problematic due to the behavior of the coefficients s (α) k with increasing k. In this paper we investigate the relations between entanglement entropies and particle fluctuations, and in particular the convergence properties of the formal expansions (5)(6)(7)(8). We will show that, in noninteracting fermion gases with N particles in a finite volume of any dimension d, the expansion (5) gets effectively truncated in the large-N limit, because the high cumulants V (n) A with n > 2 are all suppressed relatively to the particle variance…”
mentioning
confidence: 99%
“…The many-body ground state is obtained by filling the lowest N one-particle energy levels φ n (x). The cumulants V (m) A of the particle-number distribution and the entanglement entropies of a subsystem A can be written in terms of the overlap matrix [7,8] …”
mentioning
confidence: 99%