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dc.contributor.authorHsiao, Y. K.en_US
dc.contributor.authorLin, P. Y.en_US
dc.contributor.authorLih, C. C.en_US
dc.contributor.authorGeng, C. Q.en_US
dc.date.accessioned2019-04-03T06:44:37Z-
dc.date.available2019-04-03T06:44:37Z-
dc.date.issued2015-12-08en_US
dc.identifier.issn1550-7998en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.92.114013en_US
dc.identifier.urihttp://hdl.handle.net/11536/129337-
dc.description.abstractWe study the charmful decays of the two-body B-b -> BnMc decays, where B-b represents the antitriplet of (Lambda(b), Xi(0)(b), Xi(-)(b)), B-n stands for the baryon octet, and M-c denotes the charmed meson of D-(s)((*)), eta(c) and J/psi. Explicitly, we predict that B(Lambda(b) -> D(s)(-)p) = (1.8 +/- 0.3) x 10(-5), which is within the measured upper bound of B(Lambda(b) -> D(s)(-)p) < 4.8(5.3) x 10(-4) at 90% (95%) C.L., and reproduce B(Lambda(b) -> J/psi Lambda) = (3.3 +/- 2.0) x 10(-4) and B(Xi(-)(b) -> J/psi Xi(-)) = (5.1 +/- 3.2) x 10(-4) in agreement with the data. Moreover, we find that B(Lambda(b) -> Lambda eta(c)) = (1.5 +/- 0.9) x 10(-4), B(Xi(-)(b) -> Xi(-)eta(c)) = (2.4 +/- 1.5) x 10(-4) and B(Xi(0)(b) -> Xi(0)eta(c), Xi(0)J/psi) = (2.3 +/- 1.4, 4.9 +/- 3.0) x 10(-4), which are accessible to the experiments at the LHCb.en_US
dc.language.isoen_USen_US
dc.titleCharmful two-body antitriplet b-baryon decaysen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevD.92.114013en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.citation.volume92en_US
dc.citation.issue11en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000366095900003en_US
dc.citation.woscount8en_US
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