Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Hsiao, Y. K. | en_US |
dc.contributor.author | Lin, P. Y. | en_US |
dc.contributor.author | Lih, C. C. | en_US |
dc.contributor.author | Geng, C. Q. | en_US |
dc.date.accessioned | 2019-04-03T06:44:37Z | - |
dc.date.available | 2019-04-03T06:44:37Z | - |
dc.date.issued | 2015-12-08 | en_US |
dc.identifier.issn | 1550-7998 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1103/PhysRevD.92.114013 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/129337 | - |
dc.description.abstract | We 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.iso | en_US | en_US |
dc.title | Charmful two-body antitriplet b-baryon decays | en_US |
dc.type | Article | en_US |
dc.identifier.doi | 10.1103/PhysRevD.92.114013 | en_US |
dc.identifier.journal | PHYSICAL REVIEW D | en_US |
dc.citation.volume | 92 | en_US |
dc.citation.issue | 11 | en_US |
dc.citation.spage | 0 | en_US |
dc.citation.epage | 0 | en_US |
dc.contributor.department | 電子物理學系 | zh_TW |
dc.contributor.department | Department of Electrophysics | en_US |
dc.identifier.wosnumber | WOS:000366095900003 | en_US |
dc.citation.woscount | 8 | en_US |
Appears in Collections: | Articles |
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