Please use this identifier to cite or link to this item: http://hdl.handle.net/11547/11131
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dc.contributor.authorOzdem, Ulas-
dc.date.accessioned2024-03-05T06:33:40Z-
dc.date.available2024-03-05T06:33:40Z-
dc.date.issued2021-
dc.identifier.issn1434-6044-
dc.identifier.issn1434-6052-
dc.identifier.urihttp://hdl.handle.net/11547/11131-
dc.description.abstractIn this work, we employ the light-cone QCD sum rule to calculate the magnetic dipole moments of the Pc(4440), Pc(4457) and Pcs(4459) pentaquark states by considering them as the diquark-diquark-antiquark and molecular pictures with quantum numbers JP=32-, JP=12- and JP=12-, respectively. In the analyses, we use the diquark-diquark-antiquark and molecular form of interpolating currents, and photon distribution amplitudes to obtain the magnetic dipole moment of pentaquark states. Theoretical examinations on magnetic dipole moments of the hidden-charm pentaquark states, are essential as their results can help us better figure out their substructure and the dynamics of the QCD as the theory of the strong interaction. As a by product, we extract the electric quadrupole and magnetic octupole moments of the Pc(4440) pentaquark. These values show a non-spherical charge distribution.tr_TR
dc.language.isoentr_TR
dc.relation.ispartofseries81;4-
dc.subjectQCD SUM-RULEStr_TR
dc.subjectP-C(4312)tr_TR
dc.titleMagnetic dipole moments of the hidden-charm pentaquark states: Pc(4440), Pc(4457) and Pcs(4459)tr_TR
dc.typeArticletr_TR
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