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Full counting statistics in a disordered free fermion system
Full counting statistics in a disordered free fermion system
2012-01-18
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arxiv.org/abs/1201.3933v1
Physics
Condensed Matter
Mesoscale and Nanoscale Physics
6 pages, 8 figures
Scientific paper
The Full Counting Statistics (FCS) is studied for a one-dimensional system of non-interacting fermions with and without disorder. For two L-site translationally invariant lattices connected at time t=0, the charge variance increases logarithmically in t, following the universal expression ~ (1/pi^2) log t, for t much shorter than the ballistic time to encounter the boundary, t ~ L. Since the static charge variance for a length l region is given by ~ (1/pi^2) log l, this result reflects the underlying relativistic or conformal invariance and dynamical exponent z=1. With disorder and strongly localized fermions, the variance is also found to increase logarithmically in time, but with a different prefactor than in the clean case. For a small lattices, we find that the variance saturates at times t ~ t_d ~ L^2 a diffusive time scale. Despite the fact that 1-d fermions are fully localized for any disorder strength, the entanglement responsible for charge fluctuations appears to propagate with dynamical exponent z ~ 2.
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