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dc.contributor.authorCHEUNG, CYen_US
dc.contributor.authorZHANG, WMen_US
dc.contributor.authorLIN, GLen_US
dc.date.accessioned2019-04-03T06:39:04Z-
dc.date.available2019-04-03T06:39:04Z-
dc.date.issued1995-09-01en_US
dc.identifier.issn0556-2821en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.52.2915en_US
dc.identifier.urihttp://hdl.handle.net/11536/1738-
dc.description.abstractThe heavy-quark effective theory is developed on the light front. Based on this effective theory, a light-front heavy-meson bound state with definite spin and parity is constructed. Within the effective theory, the Isgur-Wise function is derived in terms of the asymptotic Light-front bound state amplitudes in the limit m(Q) --> infinity; the results a general expression for arbitrary recoil velocities. With the asymptotic form of the BSW amplitudes, the Isgur-Wise function is given by xi(upsilon .upsilon') = 1/upsilon .upsilon. The slope at the zero-recoil point is rho(2) = -xi'(1) = 1, in excellent agreement with the recent CLEO result of rho(2) = 1.01 +/- 0.15 +/- 0.09.en_US
dc.language.isoen_USen_US
dc.titleLIGHT-FRONT HEAVY-QUARK EFFECTIVE THEORY AND HEAVY-MESON BOUND-STATESen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevD.52.2915en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.citation.volume52en_US
dc.citation.issue5en_US
dc.citation.spage2915en_US
dc.citation.epage2925en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:A1995RT82200028en_US
dc.citation.woscount26en_US
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