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dc.contributor.authorDetmold, Williamen_US
dc.contributor.authorLin, C. -J. Daviden_US
dc.contributor.authorWingate, Matthewen_US
dc.date.accessioned2014-12-08T15:08:45Z-
dc.date.available2014-12-08T15:08:45Z-
dc.date.issued2009-09-01en_US
dc.identifier.issn0550-3213en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.nuclphysb.2009.03.019en_US
dc.identifier.urihttp://hdl.handle.net/11536/6695-
dc.description.abstractDynamical 2 + 1 flavour lattice QCD is used to calculate the splittings between the masses of mesons and baryons containing a single static heavy quark and domain-wall light and strange quarks. Our calculations are based on the dynamical domain-wall gauge field configurations generated by the RBC and UKQCD Collaborations at a spatial Volume of (2.7 fm)(3) and a range of quark masses with a lightest value corresponding to a (partially-quenched) pion mass of 275 MeV. When extrapolated to the physical values of the light quark masses, the results Of Our calculations are generally in good agreement with experimental determinations in the bottom sector. However, the static limit splittings between the Omega(-)(b) baryon and other bottom hadrons tend to slightly underestimate those obtained using the recent D empty set measurement of the Omega(-)(b) (C) 2009 Elsevier B.V. All rights reserved.en_US
dc.language.isoen_USen_US
dc.titleBottom hadron mass splittings in the static limit from 2+1 flavour lattice QCDen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.nuclphysb.2009.03.019en_US
dc.identifier.journalNUCLEAR PHYSICS Ben_US
dc.citation.volume818en_US
dc.citation.issue1-2en_US
dc.citation.spage17en_US
dc.citation.epage27en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000266908100002-
dc.citation.woscount7-
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