Quark ensembles with infinite correlation length
S. V. Molodtsov, G. M. Zinovjev

TL;DR
This paper develops an exactly integrable quantum field theory model of quark ensembles with infinite correlation length, revealing vacuum instabilities and supporting the BCS state as the ground state for color-interacting quarks.
Contribution
It introduces a new integrable model of quark ensembles with infinite correlation length and analyzes vacuum stability, highlighting the BCS state as the preferred ground state.
Findings
The model is exactly integrable.
Vacuum ensembles exhibit instability due to high degeneracy.
The BCS state is favored as the ground state.
Abstract
By studying quark ensembles with infinite correlation length we formulate the quantum field theory model that, as we show, is exactly integrable and develops an instability of its standard vacuum ensemble (the Dirac sea). We argue such an instability is rooted in high ground state degeneracy (for 'realistic' space-time dimensions) featuring a fairly specific form of energy distribution, and with the cutoff parameter going to infinity this inherent energy distribution becomes infinitely narrow and leads to large (unlimited) fluctuations. Analysing some possible vacuum ensembles such as the Dirac sea, neutral ensemble, color superconducting and BCS states we find out the strong arguments in favor of the BCS state as the ground state of color interacting quark ensemble.
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Taxonomy
TopicsCold Atom Physics and Bose-Einstein Condensates · Physics of Superconductivity and Magnetism · Quantum Chromodynamics and Particle Interactions
