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Electromagnetic form factors of the $B_c$-like tetraquarks: molecular and diquark-antidiquark pictures

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arxiv 2211.10169 v2 pith:VRLM6R32 submitted 2022-11-18 hep-ph hep-exhep-lat

classification hep-phhep-exhep-lat
keywords momentsmagneticlikequadrupolediquark-antidiquarkmolecularpicturesstates
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

In this study, we use the molecular and diquark-antidiquark tetraquark pictures to investigate magnetic and quadrupole moments of the $B_c$-like ground state tetraquarks with the QCD light-cone sum rules with quantum numbers $J^P = 1^+$. In the numerical analysis, to obtain the magnetic and quadrupole moments of $B_c$-like tetraquark states molecular and diquark-antidiquark forms of interpolating currents, and photon distribution amplitudes have been used. The magnetic moments are acquired as $ \mu_{Z_{{uc \bar u \bar b}}}^{Mol}=1.18^{+0.52}_{-0.40}~\mu_N$, $\mu_{Z_{{uc \bar u \bar b}}}^{Di}=3.05^{+1.19}_{-0.95}~\mu_N$, $\mu_{Z_{dc \bar d \bar b}}^{Mol}=0.32^{+0.18}_{-0.10}~\mu_N$, and $\mu_{Z_{dc \bar d \bar b}}^{Di}=2.38^{+0.95}_{-0.75}~\mu_N$. The hadrons' magnetic and quadrupole moments are another fundamental observable as their mass, which provides information on the underlying quark structure and dynamics. The results obtained in both pictures are quite different from each other. Any experimental measurement of the magnetic moments can provide an understanding of the internal structure of these states. We get nonzero but small values for the quadrupole moments of $B_c$-like tetraquark states showing non-spherical charge distributions. Hopefully, the examinations given in this study will be helpful to an experimental search of them, which will be an interesting research subject.

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Cited by 4 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. $D \bar D_1(2420)$ and $D^* \bar D^*(2400)$ molecular states: Probing their electromagnetic fingerprints

    hep-ph 2025-04 conditional novelty 6.0 of 10

    For the D \bar D_1 and D* \bar D* molecular states, the computed magnetic moments are -1.41 and 3.85 nuclear magnetons, with negative quadrupole moments, both dominated by light-quark contributions.

  2. Shedding light on the nature of the $P_{cs}(4459)$ pentaquark state

    hep-ph 2024-11 conditional novelty 5.0 of 10

    QCD light-cone sum rules with three diquark-diquark-antiquark currents predict Pcs(4459) magnetic dipole moments of -0.60, 1.60, and 0.99 nuclear magnetons.

  3. Magnetic dipole moments of the singly-heavy baryons with spin-$\frac{1}{2}$ and spin-$\frac{3}{2}$

    hep-ph 2024-11 conditional novelty 5.0 of 10

    QCD light-cone sum rules are used to predict magnetic dipole moments of all singly-heavy baryons with spin 1/2 and spin 3/2, plus electric quadrupole and magnetic octupole moments for the higher-spin states.

  4. Unveiling the electromagnetic structure and intrinsic dynamics of spin-$\frac{3}{2}$ hidden-charm pentaquarks: A comprehensive QCD analysis

    hep-ph 2025-04 conditional novelty 4.0 of 10

    QCD sum rules predict distinct magnetic dipole moments for six JP=3/2- hidden-charm pentaquarks depending on their diquark-diquark-antiquark internal structure, with the charm quark dominating the magnetic response.

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