Quantum Berezinskii-Kosterlitz-Thouless transition in the superconducting phase of (2+1)-dimensional quantum chromodynamics
Laith H. Haddad

TL;DR
This paper investigates a quantum BKT phase transition in a (2+1)-dimensional QCD model, revealing how chiral fluctuations and Fermi surface dynamics lead to the destruction of superconductivity at high density.
Contribution
It introduces a novel analysis of superconductivity and BKT transition in planar QCD using a modified Gross-Neveu model, connecting phase diagram features with chiral symmetry breaking.
Findings
Superconductivity is destroyed via a quantum BKT transition at high density.
The phase diagram aligns with other theoretical approaches.
Chiral fluctuations drive the transition and influence diquark dissolution.
Abstract
We study superconductivity in the hadron-quark mixed phase of planar quantum chromodynamics (QCD) within the large limit of a Gross-Neveu model modified by a repulsive vector term. At high densities, the combination of scalar attraction and repulsive space-like part of the vector interaction squeezes quarks into baryonic composite states, i.e., Dirac fermions with even numbers of bosonic vortices attached. The time-like vector component induces Cooper pairing between these Fermi surface modes. Remarkably, at zero temperature, competition between the quark density and mass destroys superconductivity via a Berezinskii-Kosterlitz-Thouless (BKT) phase transition driven by diverging chiral quantum fluctuations near criticality. Dissolution of logarithmically bound singlet diquarks is catalyzed by in-plane chiral mixing associated with …
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Taxonomy
TopicsQuantum Chromodynamics and Particle Interactions · Physics of Superconductivity and Magnetism · High-Energy Particle Collisions Research
