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arXiv 0706.2191hep-ph
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大N_c下稠密夸克的位相

Phases of Dense Quarks at Large N_c

Larry McLerran, Robert D. Pisarski

摘要:

在色数N_c较大的极限下,我们认为规范理论在非零温度和夸克密度下可以表现出几种不同的相。两个熟悉的:一个是冷的、稀薄的受限强子相,压力约为1;另一个是热的、非受限的夸克和胶子相,压力约为N_c^2。当夸克化学势μ ~ 1时,退凝转变温度Td与μ无关.当T < T_d时,当μ增大到质量阈值以上时,重子迅速形成压力为~ N_c的致密相。如Skyrme晶体所示,在密相中,手征对称性可以自发地被破坏,然后恢复。当压强为~ N_c时,与(非理想)夸克的压强一样,密相仍然受到限制,费米面附近的相互作用是重子的相互作用,而不是夸克的相互作用。因此在手征对称区域,费米面附近的重子是宇称加倍的。我们提出了可能的影响QCD的相图。

英文摘要:

In the limit of a large number of colors, N_c, we suggest that gauge theories can exhibit several distinct phases at nonzero temperature and quark density. Two are familiar: a cold, dilute phase of confined hadrons, where the pressure is ~ 1, and a hot phase of deconfined quarks and gluons, with pressure ~ N_c^2. When the quark chemical potential mu ~ 1, the deconfining transition temperature, T_d, is independent of mu. For T < T_d, as mu increases above the mass threshold, baryons quickly form a dense phase where the pressure is ~ N_c. As illustrated by a Skyrme crystal, chiral symmetry can be both spontaneously broken, and then restored, in the dense phase. While the pressure is ~ N_c, like that of (non-ideal) quarks, the dense phase is still confined, with interactions near the Fermi surface those of baryons, and not of quarks. Thus in the chirally symmetric region, baryons near the Fermi surface are parity doubled. We suggest possible implications for the phase diagram of QCD.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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