QCD Kondo effect for single heavy quark in chiral-symmetry broken phase

Author:

Yasui Shigehiro12ORCID,Suenaga Daiki34ORCID,Suzuki Kei5ORCID

Affiliation:

1. International Institute for Sustainability with Knotted Chiral Meta Matter (WPI-SKCM2), Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8526, Japan

2. Research and Education Center for Natural Sciences, Keio University, Hiyoshi 4-1-1, Yokohama, Kanagawa 223-8521, Japan

3. Kobayashi-Maskawa Institute for the Origin of Particles and the Universe, Nagoya University, Nagoya 464-8602, Japan

4. Research Center for Nuclear Physics, Osaka University, Ibaraki 567-0048, Japan

5. Advanced Science Research Center, Japan Atomic Energy Agency (JAEA), Tokai 319-1195, Japan

Abstract

We consider the quantum chromodynamics (QCD) Kondo effect for a single heavy quark in quark matter composed of light quarks with chiral symmetry breaking. Introducing several spinor structures in QCD Kondo condensates, i.e., particle-projected condensate, antiparticle-projected condensate, and normal condensate without projection, we calculate the attractive energy gained by the heavy quark within the mean-field approximation in the path-integral formalism. We show that the normal condensate is favored at low density and the particle-projected condensate is favored at high density, when the light quark has a nonzero mass. We interpret such a density-dependent transition between the two condensates in terms of the Kondo resonances. Published by the American Physical Society 2024

Funder

Ministry of Education, Culture, Sports, Science and Technology

RIKEN

Japan Society for the Promotion of Science

Osaka University

World Premier International Research Center Initiative

Publisher

American Physical Society (APS)

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