Charting doubly strange hidden-charm pentaquarks: An electromagnetic mapping of spin- and states
arXiv:2607.04355 · doi:10.1016/j.cjph.2026.07.002
Abstract
We calculate the magnetic dipole moments of doubly strange hidden-charm pentaquark states with spin-parity and using QCD light-cone sum rules (LCSR), presenting the first systematic LCSR investigation of the electromagnetic multipole structure in the sector. To assess the model dependence, we employ independent interpolating currents in diquark-diquark-antiquark form, which probe different assumptions about the internal color-spin correlations. For the spin- states, we also compute the electric quadrupole and magnetic octupole moments. The magnetic dipole moments exhibit a considerable spread across currents, ranging from to for spin- pentaquarks and from to for spin- states, reflecting the sensitivity of magnetic moments to the internal wave function. A quark-level decomposition reveals that the charm quark dominates in most configurations, while strange quarks play a decisive role only in currents favoring axial-vector diquark structures. The electric quadrupole moments lie between fm and fm, and the magnetic octupole moments are typically an order of magnitude smaller. The current dependence of the magnetic dipole moments provides a quantitative measure of the theoretical uncertainty arising from the choice of interpolating operator. The pronounced isospin sensitivity of across all three multipole moments arises from its axial-vector diquark structure, which isolates the light quark from spin averaging and allows the charge asymmetry to propagate directly into the electromagnetic moments; the ratio confirms this mechanism exactly. Our predictions offer benchmarks for future experiments and lattice QCD calculations, and may help discriminate among competing structural models.
22 pages, 2 figures, 4 tables. Version accepted for publication in Chinese Journal of Physics
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