Burgers-like equation for spontaneous breakdown of the chiral symmetry in QCD
arXiv:1303.2357 · doi:10.1016/j.physletb.2013.06.022
Abstract
We link the spontaneous breakdown of chiral symmetry in Euclidean QCD to the collision of spectral shock waves in the vicinity of zero eigenvalue of Dirac operator. The mechanism, originating from complex Burger's-like equation for viscid, pressureless, one-dimensional flow of eigenvalues, is similar to recently observed weak-strong coupling phase transition in large Yang-Mills theory. The spectral viscosity is proportional to the inverse of the size of the random matrix that replaces the Dirac operator in the universal (ergodic) regime. We obtain the exact scaling function and critical exponents of the chiral phase transition for the averaged characteristic polynomial for QCD. We reinterpret our results in terms of known properties of chiral random matrix models and lattice data.
12 pages
References in corpus (6)
- Chiral phase transition in lattice QCD as a metal-insulator transition
- Anderson localization through Polyakov loops: lattice evidence and Random matrix model
- Large N_c confinement and turbulence
- Burgers' equation in 2D SU(N) YM
- Non-analyticity in scale in the planar limit of QCD
- Universal shocks in the Wishart random matrix ensemble - 1
Cited by in corpus (10)
- Dysonian dynamics of the Ginibre ensemble
- Disorder in the Sachdev-Yee-Kitaev Model
- Unveiling the significance of eigenvectors in diffusing non-hermitian matrices by identifying the underlying Burgers dynamics
- On characteristic polynomials for a generalized chiral random matrix ensemble with a source
- Hydrodynamical spectral evolution for random matrices
- Diffusion method in Random Matrix Theory
- Universal shocks in the Wishart random-matrix ensemble - a sequel
- Hydrodynamics of the Chiral Dirac Spectrum
- Chiral Random Matrix Model at Finite Chemical Potential: Characteristic Determinant and Edge Universality
- Functional Equations Solving Initial-Value Problems of Complex Burgers-Type Equations for One-Dimensional Log-Gases