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On the QCD Ground State at High Density
High Energy Physics - Phenomenology · Submitted 12 Oct 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that, as previously anticipated, in the two flavor case the vacuum breaks SU(3) color to SU(2) and in the three flavor case the vacua with color-flavor locking (CFL) have the lowest energy.
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The abstract, sentence by sentence
We investigate the possible ground states of QCD at asymptotic densities, where the theory is expected to exhibit color superconductivity. We characterize the color-flavor structure of possible diquark condensates, and find those that are energy extrema by solving the weak-coupling Dyson-Schwinger equations, including Landau damping and the Meissner effect. We show that, as previously anticipated, in the two flavor case the vacuum breaks SU(3) color to SU(2) and in the three flavor case the vacua with color-flavor locking (CFL) have the lowest energy. We identify a number of relatively flat directions in the potential along which the pattern of gauge symmetry breaking changes and parity is violated. We discuss possible phenomenological consequences of our results.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the possible ground states of QCD at asymptotic densities, where the theory is expected to exhibit color superconductivity. | contribution 0.60 | 0.69 | 0.05 | hedged possibility 0.92 |
| s1 | We characterize the color-flavor structure of possible diquark condensates, and find those that are energy extrema by solving the weak-coupling Dyson-Schwinger equations, including Landau damping and the Meissner effect. | method 0.88 | 0.97 | 0.07 | asserted 1.00 |
| s2 | We show that, as previously anticipated, in the two flavor case the vacuum breaks SU(3) color to SU(2) and in the three flavor case the vacua with color-flavor locking (CFL) have the lowest energy. | result 1.00 | 0.85 | 0.70 | asserted 1.00 |
| s3 | We identify a number of relatively flat directions in the potential along which the pattern of gauge symmetry breaking changes and parity is violated. | result 0.99 | 0.94 | 0.08 | asserted 1.00 |
| s4 | We discuss possible phenomenological consequences of our results. | interpretation 0.79 | 0.73 | 0.03 | unclear 0.68 |
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The paper
Original abstract
We investigate the possible ground states of QCD at asymptotic densities, where the theory is expected to exhibit color superconductivity. We characterize the color-flavor structure of possible diquark condensates, and find those that are energy extrema by solving the weak-coupling Dyson-Schwinger equations, including Landau damping and the Meissner effect. We show that, as previously anticipated, in the two flavor case the vacuum breaks SU(3) color to SU(2) and in the three flavor case the vacua with color-flavor locking (CFL) have the lowest energy. We identify a number of relatively flat directions in the potential along which the pattern of gauge symmetry breaking changes and parity is violated. We discuss possible phenomenological consequences of our results.
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References
How the literature uses it
12 arXiv papers cite this in 19 sentences
Papers citing it · 13 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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At asymptotic densities (or equivalently, at asymptotic baryon chemical potential $μ$) and low temperatures the ground state of three flavor quark matter is the color-flavor-locked state (CFL) [ref] , where the color and flavor symmetries of QCD are broken spontaneously by a di-quark vacuum expectation value proportional to the gap parameter $Δ$, but a residual group linking color and vector flavor symmetries is left.
A diagrammatic derivation of the meson effective masses in the neutral color-flavor-locked phase of Quantum Chromodynamics · Introduction · 0.95
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From these studies [ref] we know that the ground state of three-flavor matter at asymptotically high density is the Color-Flavor Locked (CFL) phase [ref] , where quarks of all colors and flavors are paired in a homogeneous scalar ($J^P = 0^+$) diquark condensate.
NJL model of homogeneous neutral quark matter: Pseudoscalar diquark condensates revisited · Introduction · 0.95
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Various results have been obtained starting from the QCD action, employing renormalization group techniques and through the Schwinger-Dyson equation [ref] .
Crystalline color superconductors · Introduction · 0.82
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