Abstract

It was recently proposed that there is a phase in thermal QCD (IR phase) at temperatures well above the chiral crossover, featuring elements of scale invariance in the infrared (IR). Here, we study the effective spatial dimensions d_{IR} of Dirac low-energy modes in this phase, in the context of pure-glue QCD. Our d_{IR} is based on the scaling of mode support toward thermodynamic limit, and hence is an IR probe. Ordinary extended modes, such as those at high energy, have d_{IR}=3. We find d_{IR}<3 in the spectral range whose lower edge coincides with λ_{IR}=0, the singularity of spectral density defining the IR phase, and the upper edge with λ_{A}, the previously identified Anderson-like nonanalyticity. Details near λ_{IR} are unexpected in that only exact zero modes are d_{IR}=3, while a thin spectral layer near zero is d_{IR}=2, followed by an extended layer of d_{IR}=1 modes. With only integer values appearing, d_{IR} may have a topological origin. We find similar structure at λ_{A}, and associate its adjacent thin layer (d_{IR}⪆2) with Anderson-like criticality. Our analysis reveals the manner in which nonanalyticities at λ_{IR} and λ_{A}, originally identified in other quantities, appear in d_{IR}(λ). This dimension structure may be important for understanding the near-perfect fluidity of the quark-gluon medium seen in accelerator experiments. The role of λ_{A} in previously conjectured decoupling of IR component is explained.

Highlights

  • Introduction.—The interest in Dirac eigenmodes of Euclidean quantum chromodynamics (QCD) has a long history, sparked in part by the role of zero modes in topology of gauge fields (η0 problem [1]) and by that of near-zero modes in spontaneous chiral symmetry breaking (Banks-Casher relation [2])

  • While modeling of low-energy QCD based on instantons could qualitatively accommodate these features [3], the birth of numerical lattice QCD [4] allowed for computation of Dirac eigenmodes from first principles [5,6]

  • Dirac eigenmodes were used to infer the existence of a new phase in thermal QCD (IR phase) [13], showing certain signs of scale invariance at energies below temperature T

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Summary

Introduction

Introduction.—The interest in Dirac eigenmodes of Euclidean quantum chromodynamics (QCD) has a long history, sparked in part by the role of zero modes in topology of gauge fields (η0 problem [1]) and by that of near-zero modes in spontaneous chiral symmetry breaking (Banks-Casher relation [2]). This is corroborated by the finding that such a Dirac spectral feature occurs near SU(3) conformal window at zero temperature [11,14], placing both corners of the theory parameter space into one contiguous dynamical regime, the IR phase. To identify such possible connection, as well as to search for additional nonanalyticities of Dirac spectra, we study the dimension dIR 1⁄4 dIRðλÞ of spatial region effectively occupied by modes.

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