Absence of correlations in the QCD Dirac spectrum at high temperature
arXiv:0906.5373 · doi:10.1103/PhysRevLett.104.031601
Abstract
I propose a simple model of the distribution of the small eigenvalues of the QCD Dirac operator well above the finite temperature phase transition where chiral symmetry is restored and the spectral density at zero vanishes. Assuming the absence of correlations between different regions of the low lying spectrum I derive analytic formulas for the distribution of the first two eigenvalues. I find good agreement with data obtained using the overlap Dirac operator in quenched SU(2) lattice simulations. This suggests that if chiral symmetry is restored spectral correlations are not important and all the statistical properties of the spectrum are encoded in the spectral density.
4 pages, some rewording for clarification; references added
References in corpus (2)
Cited by in corpus (32)
- Hyperscaling relations in mass-deformed conformal gauge theories
- Polyakov loop modeling for hot QCD
- Microscopic Origin of \boldmath{} Symmetry Violation in the High Temperature Phase of QCD
- Anderson Localization in Quark-Gluon Plasma
- Wigner surmise for mixed symmetry classes in random matrix theory
- Anderson localization through Polyakov loops: lattice evidence and Random matrix model
- Poisson to Random Matrix Transition in the QCD Dirac Spectrum
- An Ising-Anderson model of localisation in high-temperature QCD
- Deconfinement, chiral transition and localisation in a QCD-like model
- Localization of Dirac Fermions in Finite-Temperature Gauge Theory
- Localization with overlap fermions
- Reconfinement, localization and thermal monopoles in trace-deformed Yang-Mills theory
- An Anderson-like model of the QCD chiral transition
- A Numerical Study of the 2-Flavour Schwinger Model with Dynamical Overlap Hypercube Fermions
- Lattice QCD analysis of the Polyakov loop in terms of Dirac eigenmodes
- Anderson localization in QCD-like theories
- Localisation in 2+1 dimensional SU(3) pure gauge theory at finite temperature
- Localization and chiral properties near the ordering transition of an Anderson-like toy model for QCD
- Localization properties of Dirac modes at the Roberge-Weiss phase transition
- GUE-chGUE Transition preserving Chirality at finite Matrix Size
- Localization of Dirac modes in finite-temperature gauge theory on the lattice
- Symmetry Transition Preserving Chirality in QCD: A Versatile Random Matrix Model
- Localised Dirac eigenmodes, chiral symmetry breaking, and Goldstone's theorem at finite temperature
- Deconfinement transition and localization of Dirac modes in finite-temperature gauge theory on the lattice
- Localisation of Dirac modes in gauge theories and Goldstone's theorem at finite temperature
- QCD Anderson transition with overlap valence quarks on a twisted-mass sea
- Features of a 2d Gauge Theory with Vanishing Chiral Condensate
- Level spacings for weakly asymmetric real random matrices and application to two-color QCD with chemical potential
- Quark localization in QCD above
- Spectral study of a chiral limit without chiral condensate
- High temperature quark localization by Polyakov loops
- Chiral transition, eigenmode localisation and Anderson-like models