Finite temperature free fermions and the Kardar-Parisi-Zhang equation at finite time
arXiv:1412.1590 · doi:10.1103/PhysRevLett.114.110402
Abstract
We consider the system of one-dimensional free fermions confined by a harmonic well at finite inverse temperature . The average density of fermions at position is derived. For and , is given by a scaling function interpolating between a Gaussian at high temperature, for , and the Wigner semi-circle law at low temperature, for . In the latter regime, we unveil a scaling limit, for , where the fluctuations close to the edge of the support, at , are described by a limiting kernel that depends continuously on and is a generalization of the Airy kernel, found in the Gaussian Unitary Ensemble of random matrices. Remarkably, exactly the same kernel arises in the exact solution of the Kardar-Parisi-Zhang (KPZ) equation in 1+1 dimensions at finite time , with the correspondence .
5 pages + 6 pages of supplementary material, 3 figures, published version
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- PhD thesis "Extreme value statistics of strongly correlated systems: fermions, random matrices and random walks"