Random Matrix Theory at Nonzero $μ$ and $T$

dc.creatorSplittorff, K.
dc.creatorVerbaarschot, J. J. M.
dc.date2007-04-03
dc.date.accessioned2026-07-07T11:40:56Z
dc.date.available2026-07-07T11:40:56Z
dc.descriptionWe review applications of random matrix theory to QCD at nonzero temperature and chemical potential. The chiral phase transition of QCD and QCD-like theories is discussed in terms of eigenvalues of the Dirac operator. We show that for QCD at $μ\ne 0$, which has a sign problem, the discontinuity in the chiral condensate is due to an alternative to the Banks-Casher relation. The severity of the sign problem is analyzed in the microscopic domain of QCD.
dc.descriptionInvited talk at YKIS2006, YITP-Kyoto, 10 pages, 10 figures
dc.identifierhttps://arxiv.org/abs/0704.0330
dc.identifierhttp://arxiv.org/abs/0704.0330
dc.identifierProg.Theor.Phys.Suppl.168:265-275,2007
dc.identifierdoi:10.1143/PTPS.168.265
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/200365
dc.subjectHigh Energy Physics - Phenomenology
dc.titleRandom Matrix Theory at Nonzero $μ$ and $T$
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