Please use this identifier to cite or link to this item:
https://hdl.handle.net/2440/70941
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DC Field | Value | Language |
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dc.contributor.author | Weng, M. | - |
dc.contributor.author | Guo, X. | - |
dc.contributor.author | Thomas, A. | - |
dc.date.issued | 2011 | - |
dc.identifier.citation | Physical Review D: Particles, Fields, Gravitation and Cosmology, 2011; 83(5):056006-1-056006-15 | - |
dc.identifier.issn | 1550-7998 | - |
dc.identifier.issn | 1550-2368 | - |
dc.identifier.uri | http://hdl.handle.net/2440/70941 | - |
dc.description.abstract | In the heavy quark limit, a doubly heavy baryon is regarded as composed of a heavy diquark and a light quark. We establish the Bethe-Salpeter equations for the heavy diquarks and the doubly heavy baryons, respectively, to leading order in a 1/mQ expansion. The Bethe-Salpeter equations are solved numerically under the covariant instantaneous approximation with the kernels containing scalar confinement and one-gluon-exchange terms. The masses for the heavy diquarks and the doubly heavy baryons are obtained, and the nonleptonic decay widths for the doubly heavy baryons emitting a pseudoscalar meson are calculated within the model. | - |
dc.description.statementofresponsibility | M.-H. Weng, X.-H. Guo, and A.W. Thomas | - |
dc.language.iso | en | - |
dc.publisher | American Physical Soc | - |
dc.rights | ©2011 American Physical Society | - |
dc.source.uri | http://dx.doi.org/10.1103/physrevd.83.056006 | - |
dc.title | Bethe-Salpeter equation for doubly heavy baryons in the covariant instantaneous approximation | - |
dc.type | Journal article | - |
dc.identifier.doi | 10.1103/PhysRevD.83.056006 | - |
dc.relation.grant | ARC | - |
pubs.publication-status | Published | - |
dc.identifier.orcid | Thomas, A. [0000-0003-0026-499X] | - |
Appears in Collections: | Aurora harvest 5 Physics publications |
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hdl_70941.pdf | Published version | 607.03 kB | Adobe PDF | View/Open |
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