Absence of two-flavor color-superconductivity in compact stars
Author(s) -
Mark Alford,
Krishna Rajagopal
Publication year - 2002
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/2002/06/031
Subject(s) - color superconductivity , strange matter , physics , quark star , strange quark , particle physics , pairing , quark , superconductivity , qcd matter , phase transition , phase (matter) , quantum chromodynamics , up quark , stars , color charge , down quark , color model , condensed matter physics , bottom quark , astrophysics , quantum mechanics , top quark , gluon , artificial intelligence , computer science , color space , image (mathematics)
The simplest pattern of color superconductivity involves BCS pairing betweenup and down quarks. We argue that this ``2SC'' phase will not arise within acompact star. A macroscopic volume of quark matter must be electrically neutraland must be a color singlet. Satisfying these requirements imposes asignificant free energy cost on the 2SC phase, but not on color-flavor locked(CFL) quark matter, in which up, down and strange quarks all pair. As afunction of increasing density, therefore, one may see a single phasetransition from hadronic matter directly to CFL quark matter. Alternatively,there may be an intervening phase in which the different flavors self-pair, orpair with each other in a non-BCS pattern, such as in a crystalline colorsuperconductor.Comment: Significant changes to correct an error in the derivation of the free energy for neutral CFL quark matter; result unchanged. 18 pages, 2 figure
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