Anderson Metal-to-Critical Transition in QCD
arXiv:2110.04833 · doi:10.1016/j.physletb.2022.137370
Abstract
A picture of thermal QCD phase change based on the analogy with metal-to-insulator transition of Anderson type was proposed in the past. In this picture, a low- thermal state is akin to a metal with deeply infrared (IR) Dirac modes abundant and extended, while a high- state is akin to an insulator with IR modes depleted and localized below a mobility edge . Here we argue that, while exists in QCD, a high- state is not an insulator in such an analogy. Rather, it is a critical state arising due to a new singular mobility edge at . This new mobility edge appears upon the transition into the recently proposed IR phase. As a key part of such a metal-to-critical scenario, we present evidence using pure-glue QCD that deeply infrared Dirac modes in the IR phase extend to arbitrarily long distances. This is consistent with our previous suggestion that the IR phase supports scale invariance in the infrared. We discuss the role of Anderson-like aspects in this thermal regime and emphasize that the combination of gauge field topology and disorder plays a key role in shaping its IR physics. Our conclusions are conveyed by the structure of Dirac spectral non-analyticities.
arXiv comment5 pages, 5 figures; v2: minor improvements, published version
References in corpus (22)
- Exactly massless quarks on the lattice
- Universal fluctuations in spectra of the lattice Dirac operator
- Correlated Dirac Eigenvalues and Axial Anomaly in Chiral Symmetric QCD
- Chiral Condensate in the Deconfined Phase of Quenched Gauge Theories
- Chiral phase transition in lattice QCD as a metal-insulator transition
- Anderson Localization in Quark-Gluon Plasma
- Universality and the QCD Anderson Transition
- Study of the axial U(1) anomaly at high temperature with lattice chiral fermions
- Multi-mass solvers for lattice QCD on GPUs
- Possible New Phase of Thermal QCD
- Poisson to Random Matrix Transition in the QCD Dirac Spectrum
- Eigenvalue spectra of QCD and the fate of breaking towards the chiral limit
- Chiral phase transition and Anderson localization in the Instanton Liquid Model for QCD
- Unusual Features of QCD Low-Energy Modes in IR Phase
- Anderson transition and multifractals in the spectrum of the Dirac operator of Quantum Chromodynamics at high temperature
- Phases of SU(3) Gauge Theories with Fundamental Quarks via Dirac Spectral Density
- Ideal topological gas in the high temperature phase of SU(3) gauge theory
- Effective Number Theory: Counting the Identities of a Quantum State
- Spontaneous Chiral Symmetry Breaking as Condensation of Dynamical Chirality
- The Measure Aspect of Quantum Uncertainty, of Entanglement, and the Associated Entropies
- Chiral Symmetry Breaking and Chiral Polarization: Tests for Finite Temperature and Many Flavors
- Thermal monopole condensation in QCD with physical quark masses
Cited by in corpus (8)
- Eigenvalues of the QCD Dirac matrix with improved staggered quarks in the continuum limit
- Super-Universality in Anderson Localization
- 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
- Topological Dimensions from Disorder and Quantum Mechanics?
- Understanding the approach to thermalization from the eigenspectrum of non-Abelian gauge theories
- Gluon Condensate via Dirac Spectral Density: IR Phase, Scale Anomaly and IR Decoupling