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dc.contributor.authorBilgici, Ereken_US
dc.contributor.authorFlachi, Antoninoen_US
dc.contributor.authorItou, Etsukoen_US
dc.contributor.authorKurachi, Masafumien_US
dc.contributor.authorLin, C. -J. Daviden_US
dc.contributor.authorMatsufuru, Hideoen_US
dc.contributor.authorOhki, Hiroshien_US
dc.contributor.authorOnogi, Tetsuyaen_US
dc.contributor.authorYamazaki, Takeshien_US
dc.date.accessioned2019-04-03T06:42:19Z-
dc.date.available2019-04-03T06:42:19Z-
dc.date.issued2009-08-01en_US
dc.identifier.issn1550-7998en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.80.034507en_US
dc.identifier.urihttp://hdl.handle.net/11536/6840-
dc.description.abstractWe propose a new renormalization scheme of the running coupling constant in general gauge theories using the Wilson loops. The renormalized coupling constant is obtained from the Creutz ratio in lattice simulations and the corresponding perturbative coefficient at the leading order. The latter can be calculated by adopting the zeta-function resummation techniques. We perform a benchmark test of our scheme in quenched QCD with the plaquette gauge action. The running of the coupling constant is determined by applying the step-scaling procedure. Using several methods to improve the statistical accuracy, we show that the running coupling constant can be determined in a wide range of energy scales with a relatively small number of gauge configurations.en_US
dc.language.isoen_USen_US
dc.titleNew scheme for the running coupling constant in gauge theories using Wilson loopsen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevD.80.034507en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.citation.volume80en_US
dc.citation.issue3en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000269641100064en_US
dc.citation.woscount25en_US
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