2017
DOI: 10.1016/j.aop.2017.05.018
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Periodic Airy process and equilibrium dynamics of edge fermions in a trap

Abstract: We establish an exact mapping between (i) the equilibrium (imaginary time) dynamics of noninteracting fermions trapped in a harmonic potential at temperature T = 1/β and (ii) nonintersecting Ornstein-Uhlenbeck (OU) particles constrained to return to their initial positions after time β. Exploiting the determinantal structure of the process we compute the universal correlation functions both in the bulk and at the edge of the trapped Fermi gas. The latter corresponds to the top path of the non-intersecting OU p… Show more

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Cited by 26 publications
(54 citation statements)
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References 50 publications
(172 reference statements)
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“…We find that, in a suitably tuned thermodynamic limit, our model provides a "crossover" between these two behaviors. The interpolating distribution depends on a positive parameter α and was previously encountered by Johansson in the so-called MNS random matrix model [Joh07], and by Le Doussal et al for free fermions in a confining trap [DLDMS16,LDMS17]-see also [LW17] and the discussion in Section 8. It is given explicitly by a Fredholm determinant F α psq :" detpI´M α q L 2 ps,8q , M α px, yq :" where Ai is the Airy function and α a positive parameter.…”
Section: Introductionmentioning
confidence: 84%
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“…We find that, in a suitably tuned thermodynamic limit, our model provides a "crossover" between these two behaviors. The interpolating distribution depends on a positive parameter α and was previously encountered by Johansson in the so-called MNS random matrix model [Joh07], and by Le Doussal et al for free fermions in a confining trap [DLDMS16,LDMS17]-see also [LW17] and the discussion in Section 8. It is given explicitly by a Fredholm determinant F α psq :" detpI´M α q L 2 ps,8q , M α px, yq :" where Ai is the Airy function and α a positive parameter.…”
Section: Introductionmentioning
confidence: 84%
“…Interestingly, the cylindric Plancherel measure admits a stationary continuous-time periodic extension, which is the periodic analogue of the stationary process of Borodin and Olshanski [BO06b], and which we call the cylindric Plancherel process-see Figure 2. We show that its correlation kernel converges in the edge crossover regime to the extended finite-temperature Airy kernel [LDMS17]. The cylindric Plancherel process can be thought as a certain "poissonian" limit of a measure on cylindric partitions, as described below.…”
Section: Introductionmentioning
confidence: 89%
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“…The latter problem can be studied using a mapping to non-interacting fermions in a harmonic potential (as in Ref. [43,44]). These transformations extend in the presence of a moving barrier g(τ ) = W √ τ .…”
Section: Introductionmentioning
confidence: 99%
“…This last paper has attracted much attention and it has already been cited many times in one and a half year. See, e.g., [5][6][7][8][9][10][11][12][13].…”
Section: Introductionmentioning
confidence: 99%