Please use this identifier to cite or link to this item: http://hdl.handle.net/11547/11234
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dc.contributor.authorOzdem, Ulas-
dc.date.accessioned2024-03-11T11:27:19Z-
dc.date.available2024-03-11T11:27:19Z-
dc.date.issued2020-
dc.identifier.issn1434-6001-
dc.identifier.issn1434-601X-
dc.identifier.urihttp://hdl.handle.net/11547/11234-
dc.description.abstractThe magnetic dipole moments of the spin-32 doubly charmed, bottom and charmed-bottom baryons are obtained by means of the light-cone QCD sum rule. The magnetic dipole moments of these baryons encode essential knowledge of their inner structure and shape deformations. The numerical results are given by mu Xi cc*++=2.94 +/- 0.95, mu Xi cc*+=-0.67 +/- 0.11 = - 0.67 \pm 0.11$$\end{document}, mu omega cc*+=-0.52 +/- 0.07 =- 0.52 \pm 0.07$$\end{document}, mu Xi bb*0=2.30 +/- 0.55 = 2.30 \pm 0.55$$\end{document}, mu Xi bb*-=-1.39 +/- 0.32 = -1.39 \pm 0.32$$\end{document}, mu omega bb*-=-1.56 +/- 0.33 = -1.56 \pm 0.33$$\end{document}, mu Xi bc*+=2.63 +/- 0.82 = 2.63 \pm 0.82$$\end{document}, mu Xi bc*0=-0.96 +/- 0.32 = - 0.96 \pm 0.32$$\end{document} and mu omega bc*+=-1.11 +/- 0. 33 =- 1.11 \pm 0.33$$\end{document}, respectively.tr_TR
dc.relation.ispartofseries56;2-
dc.subjectQCD SUM-RULEStr_TR
dc.subjectCHARMED BARYONStr_TR
dc.titleMagnetic dipole moments of the spin-3/2 doubly heavy baryonstr_TR
dc.typeArticletr_TR
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