Mesoscopic QCD and the \(\theta\)-vacua

DOI10.1016/S0550-3213(01)00635-6zbMath0985.81782arXivhep-th/0108166OpenAlexW2952763531MaRDI QIDQ5955497

Jonathan T. Lenaghan, Thomas Wilke

Publication date: 13 February 2002

Published in: Nuclear Physics. B (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/hep-th/0108166

zbMATH Keywords

chiral condensatepartition functionsLeutwyler-Smilga regime

Mathematics Subject Classification ID

Strong interaction, including quantum chromodynamics (81V05)

Related Items (4)

Chiral symmetry breaking with no bilinear condensate revisited ⋮ Cumulants of the QCD topological charge distribution ⋮ Singular values of the Dirac operator in dense QCD-like theories ⋮ \(\mathrm{SU}(N)\) gauge theories at large \(N\)

Cites Work

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• The microscopic spectral density of the QCD Dirac operator
• Topology and the Dirac operator spectrum in finite-volume gauge theories
• Spectral sum rules of the Dirac operator and partially quenched chiral condensates.
• Solution of the complex action problem in the Potts model for dense QCD\(^{\star}\)
• Topological susceptibility in full QCD: lattice results versus the prediction from the QCD partition function with granularity
• Phase structure of \(\mathbb{C} P^{N-1}\) model with topological term

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