Electromagnetic properties of DΛ‰(βˆ—)Ξcβ€²\bar D^{(*)}\Xi^{\prime}_c, DΛ‰(βˆ—)Ξ›c\bar D^{(*)}\Lambda_c, DΛ‰s(βˆ—)Ξ›c\bar D_s^{(*)}\Lambda_c and DΛ‰s(βˆ—)Ξc\bar D_s^{(*)}\Xi_c pentaquarks

Abstract

To elucidate the internal structure of exotic states is one of the central purposes of hadron physics. Motivated by this, we study the electromagnetic properties of DΛ‰(βˆ—)Ξcβ€²\bar D^{(*)}\Xi^{\prime}_c, DΛ‰(βˆ—)Ξ›c\bar D^{(*)}\Lambda_c, DΛ‰s(βˆ—)Ξ›c\bar D_s^{(*)}\Lambda_c and DΛ‰s(βˆ—)Ξc\bar D_s^{(*)}\Xi_c pentaquarks without strange, with strange and with double strange through QCD light-cone sum rules. We have also evaluated electric quadrupole and magnetic octupole moments of the DΛ‰βˆ—Ξžcβ€²\bar D^{*}\Xi^{\prime}_c, DΛ‰βˆ—Ξ›c\bar D^{*}\Lambda_c, DΛ‰sβˆ—Ξ›c\bar D_s^{*}\Lambda_c and DΛ‰sβˆ—Ξžc\bar D_s^{*}\Xi_c pentaquarks. The magnetic dipole moment is the leading-order response of a bound system to a soft external magnetic field. Thus, it ensures a prominent platform for the examination of the internal organizations of hadrons governed by the quark-gluon dynamics of QCD. We look forward to the present study stimulating the interest of experimentalists in investigating the electromagnetic properties of the hidden-charm pentaquarks.Comment: 20 pages, 3 tables and 2 figures. To be published in Physics Letters

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