Tuesday's seminar

Cond.Matt. & Stat.Mech.Section cm at ictp.it
Fri Mar 20 09:25:10 CET 2015


JOINT ICTP/SISSA STATISTICAL PHYSICS SEMINAR

 

Tuesday, 24 March  -   11:00 hrs.
 

Luigi Stasi Seminar Room -  ICTP Leonardo Building - 1st floor

 
Fabio FRANCHINI    (INFN - Florence Theory Section)



"Spontaneous Breaking of U (N) symmetry in  invariant Matrix Models and localization"

 
Abstract

Matrix Models have a strong history of success in describing a variety of situations, from nuclei spectra to conduction in mesoscopic systems, from strongly interacting systems to various aspects of mathematical physics. Traditionally, the requirement of base invariance has lead to a factorization of the eigenvalue and eigenvector distribution and, in turn, to the conclusion that invariant models describe extended systems. Moreover, Wigner-Dyson statistics for the eigenvalues is a hallmark of eigenvector delocalization. We show that deviations of the eigenvalue statistics from the Wigner-Dyson universality reflects itself on the eigenvector distribution and that a gap in the eigenvalue density breaks  the U(N) symmetry to a smaller one. This spontaneous symmetry breaking means that egeinvectors become localized and that the system looses ergodicity.

We also consider models with log-normal weight. Their eigenvalue distribution is intermediate between Wigner-Dyson and Poissonian, which candidates these models for describing a system intermediate between the extended and localized phase. We show that they have a much richer energy landscape than expected, with their partition functions decomposable in a large number of equilibrium configurations, growing exponentially with the matrix rank. We will discuss the meaning of this energy landscape and its implication, commenting on the perspectives for localization problems.

 
- F. Franchini; "On the Spontaneous Breaking of U(N) symmetry in invariant Matrix Models"; arXiv:1412.6523.

- F. Franchini; "Toward an invariant matrix model for the Anderson Transition"; arXiv:1503.03341.


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