Dimensional Crossover and Effective Exponents

dc.creatorLiao, Sen-Ben
dc.creatorStrickland, Michael
dc.date1996-04-22
dc.date1997-04-07
dc.date.accessioned2026-07-07T10:34:17Z
dc.date.available2026-07-07T10:34:17Z
dc.descriptionWe investigate the critical behavior of the lambda phi^4 theory defined on S^1 x R^d having two finite length scales beta, the circumference of S^1, and k^{-1}, the blocking scale introduced by the renormalization group transformation. By numerically solving the coupled differential RG equations for the finite-temperature blocked potential U_{beta,k}(Phi) and the wavefunction renormalization constant Z_{beta,k}(Phi), we demonstrate how the finite-size scaling variable betabar = beta k determines whether the phase transition is (d+1)- or d-dimensional in the limits betabar >> 1 and betabar << 1, respectively. For the intermediate values of betabar, finite-size effects play an important role. We also discuss the failure of the polynomial expansion of the effective potential near criticality.
dc.description24 pages, TeX, 8 figures in separate file, Updated version to appear in Nucl. Phys. B
dc.identifierhttps://arxiv.org/abs/hep-th/9604125
dc.identifierhttp://arxiv.org/abs/hep-th/9604125
dc.identifierNucl.Phys.B497:611-638,1997
dc.identifierdoi:10.1016/S0550-3213(97)00212-5
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/179423
dc.subjectHigh Energy Physics - Theory
dc.subjectCondensed Matter
dc.titleDimensional Crossover and Effective Exponents
dc.typetext

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