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Noncommutativity of the zero chemical potential limit and the thermodynamic limit in finite density systems

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dc.contributor.author Ambjorn, J en
dc.contributor.author Anagnostopoulos, KN en
dc.contributor.author Nishimura, J en
dc.contributor.author Verbaarschot, JJM en
dc.date.accessioned 2014-03-01T01:21:08Z
dc.date.available 2014-03-01T01:21:08Z
dc.date.issued 2004 en
dc.identifier.issn 0556-2821 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/16079
dc.subject Chemical Potential en
dc.subject Factorization Method en
dc.subject Monte Carlo Simulation en
dc.subject Qualitative Modeling en
dc.subject Random Matrix Theory en
dc.subject Thermodynamic Limit en
dc.subject Non Commutative en
dc.subject.classification Astronomy & Astrophysics en
dc.subject.classification Physics, Particles & Fields en
dc.subject.other article en
dc.subject.other density en
dc.subject.other mathematical analysis en
dc.subject.other mathematical model en
dc.subject.other Monte Carlo method en
dc.subject.other thermodynamics en
dc.title Noncommutativity of the zero chemical potential limit and the thermodynamic limit in finite density systems en
heal.type journalArticle en
heal.identifier.primary 10.1103/PhysRevD.70.035010 en
heal.identifier.secondary http://dx.doi.org/10.1103/PhysRevD.70.035010 en
heal.identifier.secondary 035010 en
heal.language English en
heal.publicationDate 2004 en
heal.abstract Monte Carlo simulations of finite density systems are often plagued by the complex action problem. We point out that there exists certain noncommutativity in the zero chemical potential limit and the thermodynamic limit when one tries to study such systems by reweighting techniques. This is demonstrated by explicit calculations in a Random Matrix Theory, which is thought to be a simple qualitative model for finite density QCD. The factorization method allows us to understand how the noncommutativity, which appears at the intermediate steps, cancels in the end results for physical observables. In the recent reweighting type of approaches to QCD in the small mu regime, we expect a transition when the volume reaches V(tr)similar or equal toconst./mu(2), which however may not be in the range of current lattice calculations. en
heal.publisher AMERICAN PHYSICAL SOC en
heal.journalName Physical Review D - Particles, Fields, Gravitation and Cosmology en
dc.identifier.doi 10.1103/PhysRevD.70.035010 en
dc.identifier.isi ISI:000223859600081 en
dc.identifier.volume 70 en
dc.identifier.issue 3 en
dc.identifier.spage 035010 en
dc.identifier.epage 1-035010-7 en


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