Pulsars as a probe for the nuclear and quark matter equation of state
Pulsars as a probe for the nuclear and quark matter equation of state
Pulsars as a probe for the nuclear and quark matter equation of state
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Ph<strong>as</strong>es in Quark Matter (Rüster et al. (2005))<br />
60<br />
50<br />
40<br />
NQ<br />
2SC<br />
uSC<br />
T [MeV]<br />
30<br />
guSC→<br />
20<br />
χSB<br />
g2SC<br />
10<br />
CFL<br />
NQ<br />
←gCFL<br />
0<br />
320 340 360 380 400 420 440 460 480 500<br />
µ [MeV]<br />
first order ph<strong>as</strong>e transition b<strong>as</strong>ed on symmetry arguments!<br />
ph<strong>as</strong>es <strong>of</strong> color superconducting <strong>quark</strong> <strong>matter</strong> in β equilibrium:<br />
normal (unpaired) <strong>quark</strong> <strong>matter</strong> (NQ)<br />
two-flavor color superconducting ph<strong>as</strong>e (2SC), gapless 2SC ph<strong>as</strong>e<br />
color-flavor locked ph<strong>as</strong>e (CFL), gapless CFL ph<strong>as</strong>e, metallic CFL ph<strong>as</strong>e<br />
(Al<strong>for</strong>d, Rajagopal, Wilczek, Reddy, Buballa, Bl<strong>as</strong>chke, Shovkovy, Drago, Rüster, Rischke,<br />
Aguilera, Banik, B<strong>and</strong>yopadhyay, Pagliara, . . . )<br />
– p.25
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