1,893 research outputs found

    U(1) axial symmetry and Dirac spectra in QCD at high temperature

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    We derive some exact results concerning the anomalous U(1)A_A symmetry in the chirally symmetric phase of QCD at high temperature. We discuss the importance of topology and finite-volume effects on the U(1)A_A symmetry violation characterized by the difference of chiral susceptibilities. In particular, we present a reliable method to measure the anomaly strength in lattice simulations with fixed topology. We also derive new spectral sum rules and a novel Banks-Casher-type relation. Through our spectral analysis we arrive at a simple alternative proof of the Aoki-Fukaya-Taniguchi "theorem" on the effective restoration of the U(1)A_A symmetry at high temperature.Comment: 28 pages, 2 figures; v2: Section 2 was substantially rewritten and Section 4 was omitted. published versio

    Banks-Casher-type relation for the BCS gap at high density

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    We derive a new Banks-Casher-type relation which relates the density of complex Dirac eigenvalues at the origin to the BCS gap of quarks at high density. Our relation is applicable to QCD and QCD-like theories without a sign problem, such as two-color QCD and adjoint QCD with baryon chemical potential, and QCD with isospin chemical potential. It provides us with a method to measure the BCS gap through the Dirac spectrum on the lattice.Comment: 14 pages, 2 figures, some additions (in particular eq. (4.13)), version to appear in EPJ

    Banks-Casher-type relations for complex Dirac spectra

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    For theories with a sign problem there is no analog of the Banks-Casher relation. This is true in particular for QCD at nonzero quark chemical potential. However, for QCD-like theories without a sign problem the Banks-Casher relation can be extended to the case of complex Dirac eigenvalues. We derive such extensions for the zero-temperature, high-density limits of two-color QCD, QCD at nonzero isospin chemical potential, and adjoint QCD. In all three cases the density of the complex Dirac eigenvalues at the origin is proportional to the BCS gap squared.Comment: 7 pages, talk presented at Lattice 201
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