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On gap equations and color-flavor locking in cold dense QCD with three massless flavors
High Energy Physics - Phenomenology · Submitted 4 Oct 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is shown that the antitriplet-antitriplet gives the dominant contribution to the color-flavor locked order parameter, while the sextet-sextet is small but nonzero.
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The abstract, sentence by sentence
The superconductivity in cold dense QCD with three massless flavors is analyzed in the framework of the Schwinger-Dyson equation. The set of two coupled gap equations for the color antitriplet, flavor antitriplet (bar{3},bar{3}) and the color sextet, flavor sextet (6,6) order parameters is derived. It is shown that the antitriplet-antitriplet gives the dominant contribution to the color-flavor locked order parameter, while the sextet-sextet is small but nonzero.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The superconductivity in cold dense QCD with three massless flavors is analyzed in the framework of the Schwinger-Dyson equation. | method 0.59 | 0.83 | 0.05 | asserted 0.97 |
| s1 | The set of two coupled gap equations for the color antitriplet, flavor antitriplet (bar{3},bar{3}) and the color sextet, flavor sextet (6,6) order parameters is derived. | contribution 0.67 | 0.91 | 0.08 | asserted 1.00 |
| s2 | It is shown that the antitriplet-antitriplet gives the dominant contribution to the color-flavor locked order parameter, while the sextet-sextet is small but nonzero. | result 1.00 | 0.91 | 0.80 | asserted 1.00 |
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The paper
Original abstract
The superconductivity in cold dense QCD with three massless flavors is analyzed in the framework of the Schwinger-Dyson equation. The set of two coupled gap equations for the color antitriplet, flavor antitriplet (bar{3},bar{3}) and the color sextet, flavor sextet (6,6) order parameters is derived. It is shown that the antitriplet-antitriplet gives the dominant contribution to the color-flavor locked order parameter, while the sextet-sextet is small but nonzero.
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References
How the literature uses it
10 arXiv papers cite this in 12 sentences
Papers citing it · 6 sentences without a confident label
Cites it as support 1 paper
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This has been confirmed by weak-coupling QCD calculations [ref] , Dyson-Schwinger calculations [ref] , and in Nambu–Jona-Lasinio models [ref] .
Quark matter in neutron stars · Color-flavor locking (CFL) · 0.98
Cites it as background 5 papers
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Theoretically, some results have been already obtained on a sound basis: First, the lattice simulations of quantum chromodynamics (QCD) indicate that, for physical quark masses, the transition from the hadronic phase to the quark gluon plasma (QGP) is a smooth crossover at finite temperature and vanishing baryon chemical potential [ref] , whereas in the low temperature and very high density region, the techniques of perturbation QCD can be used and the color flavor locking (CFL) [ref] phase is proved to be the ground state of QCD [ref] .
Roles of axial anomaly on neutral quark matter with color superconducting phase · INTRODUCTION · 0.92
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In this work, we compute $χ$ in superdense phases of QCD, in which the system could be in a color-superconductive phase [ref] .
Topological Susceptibility in the Superconductive Phases of Quantum Chromodynamics: a Dyson-Schwinger Perspective · Introduction · 0.92
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At high densities, the color-flavor locked (CFL) phase [ref] , in which all three colors (red, green, blue) and all three flavors (up, down, strange) are paired is the energetically favored phase [ref] .
Astrophysical constraints on color-superconducting phases in compact stars within the RG-consistent NJL model · Introduction · 0.81
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