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dc.contributor.authorLi, HNen_US
dc.contributor.authorLin, GLen_US
dc.date.accessioned2019-04-03T06:39:11Z-
dc.date.available2019-04-03T06:39:11Z-
dc.date.issued1999-09-01en_US
dc.identifier.issn0556-2821en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.60.054001en_US
dc.identifier.urihttp://hdl.handle.net/11536/31097-
dc.description.abstractWe apply the perturbative QCD factorization theorem developed recently for nonleptonic heavy meson decays to the radiative decay B-->K* gamma. In this formalism the evolution of the Wilson coefficients from the W boson mass down to the characteristic scale of the decay process is governed by the effective weak Hamiltonian. The evolution from the characteristic scale to a lower hadronic scale is formulated by the Sudakov resummation. In addition to computing the dominant contribution arising from the magnetic-penguin operator O-7. We also calculate the contributions of four-quark operators. By fitting our prediction for the branching ratio of the B-->K* gamma decay to the CLEO data, we determine the B meson wave function that possesses a sharp peak at a low momentum fraction. [S0556-2821(99)01015-2].en_US
dc.language.isoen_USen_US
dc.titlePerturbative QCD study of the B -> K* gamma decayen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevD.60.054001en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.citation.volume60en_US
dc.citation.issue5en_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:000082470200019en_US
dc.citation.woscount14en_US
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