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arxiv: 2510.18492 · v3 · submitted 2025-10-21 · ✦ hep-ph · hep-ex

Electromagnetic characteristics as probes into the inner structures of the predicted Xi_c^((',*))D^((*))_s molecular states

Pith reviewed 2026-05-18 05:14 UTC · model grok-4.3

classification ✦ hep-ph hep-ex
keywords molecular pentaquarkselectromagnetic propertiesmagnetic momentsM1 radiative decaysdouble-charm stateshidden strangenessconstituent quark modelexotic hadrons
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0 comments X

The pith

Magnetic moments and M1 decays of predicted double-charm hidden-strangeness molecular pentaquarks display patterns that distinguish their constituent configurations and quantum numbers.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper calculates magnetic moments and M1 radiative decay widths for the predicted Ξ_c^{(',*)}D^{(*)}_s molecular pentaquarks inside the constituent quark model. It performs the work in three scenarios: single-channel, S-D wave mixing, and coupled-channel. The magnetic moments produce patterns that track the underlying quark configurations and serve as diagnostics for quantum number assignments. Several M1 channels appear with widths large enough to be observable and to further separate different possible internal structures.

Core claim

The calculated magnetic moments reveal characteristic patterns that reflect their underlying constituent configurations and provide sensitive probes for their quantum number assignments. Furthermore, several M1 radiative decay channels with sizable widths are identified that may offer promising signatures for future experimental detection. These M1 transitions also act as sensitive probes into their inner structures, displaying distinctive features that help differentiate between their constituent configurations and quantum number assignments.

What carries the argument

Constituent quark model evaluation of magnetic moments and M1 radiative transitions performed in single-channel, S-D mixing, and coupled-channel treatments

If this is right

  • Magnetic moments form patterns tied directly to specific constituent quark configurations.
  • Quantum number assignments can be tested by comparing measured moments against the predicted patterns.
  • Several M1 radiative channels carry widths large enough to serve as experimental search channels.
  • M1 transition rates display features that separate one configuration or assignment from another.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Confirmation of the predicted moment patterns would favor a molecular picture over compact multiquark alternatives for these states.
  • The same electromagnetic observables could be computed for other predicted molecular pentaquarks to build a systematic map of their structures.
  • Targeted searches for the identified M1 channels at existing or future heavy-flavor experiments would directly test the model results.

Load-bearing premise

The constituent quark model remains valid and accurate enough to describe the electromagnetic properties of these loosely bound molecular pentaquarks and the existence of the predicted states with assigned quantum numbers.

What would settle it

A measured magnetic moment or M1 width for any of these states that lies outside the range of all values computed across the three analysis scenarios and possible quantum number assignments.

Figures

Figures reproduced from arXiv: 2510.18492 by Fu-Lai Wang, Sheng-He Zhu, Xiang Liu.

Figure 1
Figure 1. Figure 1: FIG. 1: The spatial wave functions [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: The magnetic moments [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: The magnetic moments [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: The magnetic moments [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
read the original abstract

In this work, we conduct a systematic investigation of the electromagnetic properties, specifically the magnetic moments and the M1 radiative decay behavior, of the predicted $\Xi_c^{(',*)}D^{(*)}_s$-type double-charm hidden-strangeness molecular pentaquarks. The study is carried out within the framework of the constituent quark model to evaluate these electromagnetic observables, and our analysis incorporates three distinct scenarios: single-channel analysis, $S$-$D$ wave mixing analysis, and coupled-channel analysis. The calculated magnetic moments reveal characteristic patterns that reflect their underlying constituent configurations and provide sensitive probes for their quantum number assignments. Furthermore, we identify several M1 radiative decay channels with sizable widths that may offer promising signatures for future experimental detection. These M1 transitions also act as sensitive probes into their inner structures, displaying distinctive features that help differentiate between their constituent configurations and quantum number assignments. We anticipate that this study will stimulate experimental interest in exploring the electromagnetic properties of the $\Xi_c^{(',*)}D^{(*)}_s$ molecular states, thereby advancing our structural understanding of these exotic hadronic states.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript calculates magnetic moments and M1 radiative decay widths for the predicted Ξ_c^{(',*)}D_s^{(*)} molecular pentaquarks within the constituent quark model. Three scenarios are considered: single-channel, S-D wave mixing, and coupled-channel. The authors report that the magnetic moments exhibit configuration-specific patterns that can serve as probes for quantum number assignments, and they identify several M1 transitions with sizable widths that could be observable experimentally and further distinguish inner structures.

Significance. If the results hold, the work would supply concrete electromagnetic observables that could help discriminate among possible assignments for these double-charm hidden-strangeness states and motivate targeted experimental searches. The provision of results across multiple mixing scenarios is a positive feature that allows internal consistency checks.

major comments (2)
  1. [Formalism and Results sections] The central claim that the calculated magnetic moments and M1 widths provide reliable probes into the inner structures rests on the applicability of the constituent quark model to loosely bound molecular states. The manuscript performs single-channel, S-D mixing, and coupled-channel calculations but does not demonstrate that the electromagnetic operators remain stable when the spatial wave function is extended to the molecular scale set by the small binding momentum, where long-range hadronic currents would dominate over short-distance quark currents.
  2. [Formalism] The constituent quark model parameters (masses and couplings) are typically fitted to known hadron properties. Without an explicit discussion of how the reported magnetic moments and widths depend on or are independent of those prior fits, it is unclear whether the characteristic patterns are genuine predictions or largely inherited from the input fits.
minor comments (2)
  1. [Results] The abstract states that 'several M1 radiative decay channels with sizable widths' are identified, but the main text should tabulate the numerical widths together with the corresponding transition matrix elements and phase-space factors for each channel and each scenario.
  2. [Introduction] Notation for the states (e.g., Ξ_c^{(',*)}D^{(*)}_s) should be defined once at the beginning and used consistently; occasional shifts between primed and unprimed labels make cross-referencing the three scenarios harder.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address each major point below and will revise the manuscript to strengthen the discussion of model applicability and parameter sensitivity.

read point-by-point responses
  1. Referee: [Formalism and Results sections] The central claim that the calculated magnetic moments and M1 widths provide reliable probes into the inner structures rests on the applicability of the constituent quark model to loosely bound molecular states. The manuscript performs single-channel, S-D mixing, and coupled-channel calculations but does not demonstrate that the electromagnetic operators remain stable when the spatial wave function is extended to the molecular scale set by the small binding momentum, where long-range hadronic currents would dominate over short-distance quark currents.

    Authors: We acknowledge the importance of justifying the use of quark-level electromagnetic operators for states with small binding momenta. In our framework the molecular wave functions are obtained by solving the Schrödinger equation with a phenomenological potential, and the magnetic moment and M1 operators act on the constituent quarks while the relative orbital motion is included explicitly. This is the standard procedure employed in constituent-quark-model studies of hadronic molecules. Nevertheless, we agree that an explicit discussion of the approximation is warranted. We will add a paragraph in the Formalism section that (i) recalls the typical binding momenta of the states under consideration, (ii) notes that the dominant contribution to the magnetic moments still arises from the short-distance quark currents, and (iii) states the limitation that long-range meson-exchange currents are not included and could provide O(10–20 %) corrections. This addition will clarify the range of validity without altering the reported patterns. revision: yes

  2. Referee: [Formalism] The constituent quark model parameters (masses and couplings) are typically fitted to known hadron properties. Without an explicit discussion of how the reported magnetic moments and widths depend on or are independent of those prior fits, it is unclear whether the characteristic patterns are genuine predictions or largely inherited from the input fits.

    Authors: The quark masses and magnetic-moment parameters are taken from well-established literature fits that reproduce the spectra and magnetic moments of conventional mesons and baryons. The configuration-specific patterns we obtain originate from the different ways the individual quark magnetic moments and orbital angular momenta combine according to the total quantum numbers of each molecular state. To make this robustness explicit, we will insert a short subsection (or paragraph) in the Formalism section that reports the results of a limited parameter variation (changing quark masses by ±10 % and the anomalous magnetic moments within their conventional ranges) and shows that the qualitative ordering and relative sizes of the magnetic moments remain unchanged. This will demonstrate that the reported patterns are driven by the constituent structure rather than by fine details of the input fits. revision: yes

Circularity Check

0 steps flagged

No significant circularity; model outputs are independent of target observables

full rationale

The paper applies the constituent quark model to compute magnetic moments and M1 decay widths for the predicted states using single-channel, S-D mixing, and coupled-channel analyses. The abstract and available text present these as calculated results that reveal patterns and serve as probes, without any quoted equations or statements reducing the outputs to self-definitions, direct fits to the same observables, or load-bearing self-citations that make the central claims tautological. The derivation remains self-contained against the model's standard assumptions and external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the applicability of the constituent quark model to molecular pentaquarks and on standard model parameters that are typically adjusted to reproduce known hadron properties.

free parameters (1)
  • constituent quark masses and couplings
    Quark-model calculations of magnetic moments and radiative widths require input values for quark masses and effective couplings that are fitted to conventional hadrons.
axioms (1)
  • domain assumption Constituent quark model accurately captures electromagnetic observables for molecular states
    The study is carried out within the framework of the constituent quark model.

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discussion (0)

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Forward citations

Cited by 2 Pith papers

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

  1. Deciphering the nature of $P^{\Sigma}_{\psi s}$ pentaquarks in the light of their electromagnetic multipole moments

    hep-ph 2026-04 unverdicted novelty 7.0

    Electromagnetic moments of Σ-type pentaquarks are computed via light-cone sum rules, yielding flavor-sensitive magnetic dipoles, quadrupoles, and octupoles that distinguish diquark types and rule out S-wave molecules.

  2. Deciphering the nature of $P^{\Sigma}_{\psi s}$ pentaquarks in the light of their electromagnetic multipole moments

    hep-ph 2026-04 unverdicted novelty 6.0

    QCD light-cone sum rules computation of magnetic dipole, electric quadrupole, and magnetic octupole moments for Σ-type P_ψs pentaquarks, with quark-flavor decomposition and model discriminants.

Reference graph

Works this paper leans on

176 extracted references · 176 canonical work pages · cited by 1 Pith paper · 1 internal anchor

  1. [1]

    Electromagnetic characteristics as probes into the inner structures of the predicted $\Xi_c^{(',*)}D^{(*)}_s$ molecular states

    andP Λ ψs(4338) existing in theJ/ψΛinvariant mass spectrum [22], interpretable as theΞ c ¯D∗ andΞ c ¯Dmolecu- lar candidates, respectively [23–63]. In addition, the 2022 discovery of the double-charm tetraquark stateT cc(3875)+ [64, 65], explained as aDD ∗ molecular candidate [66–109], further enriched this picture. The experimental observations of the hi...

  2. [2]

    It should be noted that the color wave function of a hadronic molecular state is taken as a color singlet

    single-channel analysis To calculating the magnetic moments of theΞ (′,∗) c D(∗) s molecular pentaquarks, we begin by constructing their flavor and spin wave functions. It should be noted that the color wave function of a hadronic molecular state is taken as a color singlet. Furthermore, in single-channel analysis, the spatial wave function is required to...

  3. [3]

    S -D wave mixing analysis We now extend our analysis of the magnetic moments for the predictedΞ (′,∗) c D(∗) s molecular states by incorporat- ing contributions from theD-wave channels. It should be noted that the tensor force is absent in the interactions of the ΞcD∗ s andΞ ∗ cDs systems [112], theD-wave channel contri- bution is consequently zero in bot...

  4. [4]

    Coupled-channel analysis Having systematically analyzed the magnetic moment properties of theΞ(′,∗) c D(∗) s molecular pentaquarks through both single-channel analysis andS-Dwave mixing analysis, we now proceed to include coupled-channel effects in our inves- tigation. For theΞ cDs state withJ P =1/2 − and theΞ cD∗ s state withJ P =3/2 −, when coupled-cha...

  5. [5]

    Liu, An overview ofXYZnew particles, Chin

    X. Liu, An overview ofXYZnew particles, Chin. Sci. Bull. 59, 3815 (2014)

  6. [6]

    Karliner and J

    M. Karliner and J. L. Rosner, New Exotic Meson and Baryon Resonances from Doubly-Heavy Hadronic Molecules, Phys. Rev. Lett.115, 122001 (2015)

  7. [7]

    Hosaka, T

    A. Hosaka, T. Iijima, K. Miyabayashi, Y . Sakai, and S. Yasui, Exotic hadrons with heavy flavors:X,Y,Z, and related states, Prog. Theor. Exp. Phys.2016, 062C01 (2016)

  8. [8]

    J. M. Richard, Exotic hadrons: review and perspectives, Few- Body Syst.57, 1185 (2016)

  9. [9]

    H. X. Chen, W. Chen, X. Liu, and S. L. Zhu, The hidden- charm pentaquark and tetraquark states, Phys. Rep.639, 1 (2016)

  10. [10]

    R. F. Lebed, R. E. Mitchell, and E. S. Swanson, Heavy-Quark QCD Exotica, Prog. Part. Nucl. Phys.93, 143 (2017)

  11. [11]

    S. L. Olsen, T. Skwarnicki, and D. Zieminska, Nonstan- dard heavy mesons and baryons: Experimental evidence, Rev. Mod. Phys.90, 015003 (2018)

  12. [12]

    F. K. Guo, C. Hanhart, U. G. Meißner, Q. Wang, Q. Zhao, and B. S. Zou, Hadronic molecules, Rev. Mod. Phys.90, 015004 (2018)

  13. [13]

    Y . R. Liu, H. X. Chen, W. Chen, X. Liu, and S. L. Zhu, Pen- taquark and tetraquark states, Prog. Part. Nucl. Phys.107, 237 (2019)

  14. [14]

    Brambilla, S

    N. Brambilla, S. Eidelman, C. Hanhart, A. Nefediev, C. P. Shen, C. E. Thomas, A. Vairo, and C. Z. Yuan, TheXYZ states: Experimental and theoretical status and perspectives, Phys. Rep.873, 1 (2020)

  15. [15]

    L. Meng, B. Wang, G. J. Wang, and S. L. Zhu, Chiral perturba- tion theory for heavy hadrons and chiral effective field theory for heavy hadronic molecules, Phys. Rep.1019, 1 (2023)

  16. [16]

    H. X. Chen, W. Chen, X. Liu, Y . R. Liu, and S. L. Zhu, An updated review of the new hadron states, Rep. Prog. Phys.86, 026201 (2023)

  17. [17]

    M. Z. Liu, Y . W. Pan, Z. W. Liu, T. W. Wu, J. X. Lu, and L. S. Geng, Three ways to decipher the nature of exotic hadrons: Multiplets, three-body hadronic molecules, and cor- relation functions, Phys. Rep.1108, 1 (2025)

  18. [18]

    Z. G. Wang, Review of the QCD sum rules for exotic states, Front. Phys.21, 016300 (2026)

  19. [19]

    S. K. Choiet al.(Belle Collaboration), Observation of a Nar- row Charmonium-Like State in ExclusiveB ± →K ±π+π− J/ψ Decays, Phys. Rev. Lett.91, 262001 (2003)

  20. [20]

    Aaijet al.(LHCb Collaboration), Observation of a narrow pentaquark state,P c(4312)+, and of two-peak structure of the Pc(4450)+, Phys

    R. Aaijet al.(LHCb Collaboration), Observation of a narrow pentaquark state,P c(4312)+, and of two-peak structure of the Pc(4450)+, Phys. Rev. Lett.122, 222001 (2019)

  21. [21]

    J. J. Wu, R. Molina, E. Oset, and B. S. Zou, Prediction of narrowN ∗ andΛ ∗ resonances with hidden charm above 4 GeV , Phys. Rev. Lett.105, 232001 (2010)

  22. [22]

    W. L. Wang, F. Huang, Z. Y . Zhang, and B. S. Zou,Σ c ¯Dand Λc ¯Dstates in a chiral quark model, Phys. Rev. C84, 015203 (2011)

  23. [23]

    Z. C. Yang, Z. F. Sun, J. He, X. Liu, and S. L. Zhu, The possible hidden-charm molecular baryons composed of anti- charmed meson and charmed baryon, Chin. Phys. C36, 6 (2012)

  24. [24]

    J. J. Wu, T. S. H. Lee, and B. S. Zou, Nucleon resonances with hidden charm in coupled-channel Models, Phys. Rev. C85, 044002 (2012)

  25. [25]

    Aaijet al.(LHCb Collaboration), Evidence of aJ/ψΛ structure, and observation of excitedΞ − states in theΞ − b → J/ψΛK − decay, Sci

    R. Aaijet al.(LHCb Collaboration), Evidence of aJ/ψΛ structure, and observation of excitedΞ − states in theΞ − b → J/ψΛK − decay, Sci. Bull.66, 1278 (2021)

  26. [26]

    Aaijet al.(LHCb Collaboration), Observation of aJ/ψΛ resonance consistent with a strange pentaquark candidate in B− →J/ψΛ¯pdecays, Phys

    R. Aaijet al.(LHCb Collaboration), Observation of aJ/ψΛ resonance consistent with a strange pentaquark candidate in B− →J/ψΛ¯pdecays, Phys. Rev. Lett.131, 031901 (2023)

  27. [27]

    Hofmann and M

    J. Hofmann and M. F. M. Lutz, Coupled-channel study of crypto-exotic baryons with charm, Nucl. Phys. A763, 90 (2005)

  28. [28]

    J. J. Wu, R. Molina, E. Oset, and B. S. Zou, Dynamically generatedN ∗ andΛ ∗ resonances in the hidden charm sector around 4.3 GeV , Phys. Rev. C84, 015202 (2011)

  29. [29]

    V . V . Anisovich, M. A. Matveev, J. Nyiri, A. V . Sarantsev, and A. N. Semenova, Nonstrange and strange pentaquarks with hidden charm, Int. J. Mod. Phys. A30, 1550190 (2015)

  30. [30]

    R. Chen, J. He, and X. Liu, Possible strange hidden-charm pentaquarks fromΣ (∗) c ¯D∗ s andΞ (′,∗) c ¯D∗ interactions, Chin. Phys. C41, 103105 (2017)

  31. [31]

    X. Z. Weng, X. L. Chen, W. Z. Deng, and S. L. Zhu, Hidden- charm pentaquarks andP c states, Phys. Rev. D100, 016014 (2019)

  32. [32]

    C. W. Xiao, J. Nieves, and E. Oset, Prediction of hidden charm strange molecular baryon states with heavy quark spin sym- metry, Phys. Lett. B799, 135051 (2019)

  33. [33]

    B. Wang, L. Meng, and S. L. Zhu, Spectrum of the strange hidden charm molecular pentaquarks in chiral effective field theory, Phys. Rev. D101, 034018 (2020)

  34. [34]

    H. X. Chen, W. Chen, X. Liu, and X. H. Liu, Establishing the first hidden-charm pentaquark with strangeness, Eur. Phys. J. C81, 409 (2021)

  35. [35]

    M. L. Du, Z. H. Guo, and J. A. Oller, Insights into the nature 11 of theP cs(4459), Phys. Rev. D104, 114034 (2021)

  36. [36]

    X. K. Dong, F. K. Guo, and B. S. Zou, A survey of heavy- antiheavy hadronic molecules, Progr. Phys.41, 65 (2021)

  37. [37]

    J. X. Lu, M. Z. Liu, R. X. Shi, and L. S. Geng, Understanding Pcs(4459) as a hadronic molecule in theΞ− b →J/ψΛK − decay, Phys. Rev. D104, 034022 (2021)

  38. [38]

    B. S. Zou, Building up the spectrum of pentaquark states as hadronic molecules, Sci. Bull.66, 1258 (2021)

  39. [39]

    Z. G. Wang and Q. Xin, Analysis of hidden-charm pentaquark molecular states with and without strangeness via the QCD sum rules, Chin. Phys. C45, 123105 (2021)

  40. [40]

    F. Z. Peng, M. J. Yan, M. S´anchez S´anchez, and M. P. Valder- rama, TheP cs(4459) pentaquark from a combined effective field theory and phenomenological perspective, Eur. Phys. J. C81, 666 (2021)

  41. [41]

    J. T. Zhu, L. Q. Song, and J. He,P cs(4459) and other possible molecular states fromΞ (∗) c ¯D(∗) andΞ ′ c ¯D(∗) interactions, Phys. Rev. D103, 074007 (2021)

  42. [42]

    Z. G. Wang, Analysis of theP cs(4459) as the hidden-charm pentaquark state with QCD sum rules, Int. J. Mod. Phys. A 36, 2150071 (2021)

  43. [43]

    Chen, Can the newly reportedP cs(4459) be a strange hidden-charmΞ c ¯D∗ molecular pentaquark?, Phys

    R. Chen, Can the newly reportedP cs(4459) be a strange hidden-charmΞ c ¯D∗ molecular pentaquark?, Phys. Rev. D103, 054007 (2021)

  44. [44]

    C. W. Xiao, J. J. Wu, and B. S. Zou, Molecular nature of Pcs(4459) and its heavy quark spin partners, Phys. Rev. D103, 054016 (2021)

  45. [45]

    K. Chen, R. Chen, L. Meng, B. Wang, and S. L. Zhu, System- atics of the heavy flavor hadronic molecules, Eur. Phys. J. C 82, 581 (2022)

  46. [46]

    Chen and X

    R. Chen and X. Liu, Mass behavior of hidden-charm open- strange pentaquarks inspired by the establishedP c molecular states, Phys. Rev. D105, 014029 (2022)

  47. [47]

    K. Chen, B. Wang, and S. L. Zhu, Heavy flavor molecular states with strangeness, Phys. Rev. D105, 096004 (2022)

  48. [48]

    Hu and J

    X. Hu and J. Ping, Investigation of hidden-charm pentaquarks with strangenessS=−1, Eur. Phys. J. C82, 118 (2022)

  49. [49]

    Garcilazo and A

    H. Garcilazo and A. Valcarce, Hidden-flavor pentaquarks, Phys. Rev. D106, 114012 (2022)

  50. [50]

    K. Chen, Z. Y . Lin, and S. L. Zhu, Comparison between the PN ψ andP Λ ψs systems, Phys. Rev. D106, 116017 (2022)

  51. [51]

    Karliner and J

    M. Karliner and J. R. Rosner, strange pentaquarks, Phys. Rev. D106, 036024 (2022)

  52. [52]

    F. L. Wang and X. Liu, Emergence of molecular-type characteristic spectrum of hidden-charm pentaquark with strangeness embodied in theP Λ ψs(4338) andP cs(4459), Phys. Lett. B835, 137583 (2022)

  53. [53]

    F. Z. Peng, M. Z. Liu, Y . W. Pan, M. S ´anchez S ´anchez, and M. Pavon Valderrama, Five-flavor pentaquarks and other light- and heavy-flavor symmetry partners of the LHCb hidden- charm pentaquarks, Nucl. Phys. B983, 115936 (2022)

  54. [54]

    C. W. Xiao, J. Nieves, E. Oset, J. J. Wu, and B. S. Zou, Is Pcs(4459) one state or two?, Rev. Mex. Fis. Suppl.3, 0308045 (2022)

  55. [55]

    X. W. Wang and Z. G. Wang, Study of isospin eigenstates of the pentaquark molecular states with strangeness, Int. J. Mod. Phys. A37, 2250189 (2022)

  56. [56]

    Clymton, H

    S. Clymton, H. J. Kim, and H. C. Kim, The effect of hidden- charm strange pentaquarksp cs on theK − p→J/ψΛreaction, Rev. Mex. Fis. Suppl.3, 0308040 (2022)

  57. [57]

    Ferretti and E

    J. Ferretti and E. Santopinto, The newP cs(4459),Z cs(3985), Zcs(4000) andZ cs(4220) and the possible emergence of flavor pentaquark octets and tetraquark nonets, Sci. Bull.67, 1209 (2022)

  58. [58]

    Giachino, A

    A. Giachino, A. Hosaka, E. Santopinto, S. Takeuchi, M. Tak- izawa, and Y . Yamaguchi, Rich structure of the hidden-charm pentaquarks near threshold regions, Phys. Rev. D108, 074012 (2023)

  59. [59]

    S. X. Nakamura and J. J. Wu, Pole determination ofP Λ ψs(4338) and possibleP Λ ψs(4255) inB − →J/ψΛ¯p, Phys. Rev. D108, L011501 (2023)

  60. [60]

    M. J. Yan, F. Z. Peng, M. S ´anchez S ´anchez, and M. Pavon Valderrama,P Λ ψs(4338) pentaquark and its partners in the molecular picture, Phys. Rev. D107, 074025 (2023)

  61. [61]

    Azizi, Y

    K. Azizi, Y . Sarac, and H. Sundu, Investigation of the strange pentaquark candidateP Λ ψs(4338)0 recently observed by LHCb, arXiv:2304.00604

  62. [62]

    Feijoo, W

    A. Feijoo, W. F. Wang, C. W. Xiao, J. J. Wu, E. Oset, J. Nieves, and B. S. Zou, A new look at theP cs states from a molecular perspective, Phys. Lett. B839, 137760 (2023)

  63. [63]

    J. T. Zhu, S. Y . Kong, and J. He,P Λ ψs(4459) andP Λ ψs(4338) as molecular states inJ/ψΛinvariant mass spectra, Phys. Rev. D 107, 034029 (2023)

  64. [64]

    P. G. Ortega, D. R. Entem, and F. Fernandez, Strange hidden- charmP Λ ψs(4459) andP Λ ψs(4338) pentaquarks and additional PΛ ψs,P Σ ψs andP N ψss candidates in a quark model approach, Phys. Lett. B838, 137747 (2023)

  65. [65]

    L. Meng, B. Wang, and S. L. Zhu, Double thresholds distort the line shapes of theP Λ ψs(4338)0 resonance, Phys. Rev. D107, 014005 (2023)

  66. [66]

    X. W. Wang and Z. G. Wang, Analysis ofP cs(4338) and re- lated pentaquark molecular states via QCD sum rules, Chin. Phys. C47, 013109 (2023)

  67. [67]

    Z. Y . Yang, F. Z. Peng, M. J. Yan, M. S ´anchez S´anchez, and M. Pavon Valderrama, MolecularP ψ pentaquarks from light- meson exchange saturation, Phys. Rev. D111, 014012 (2025)

  68. [68]

    Aaijet al.(LHCb Collaboration), Observation of an exotic narrow doubly charmed tetraquark, Nat

    R. Aaijet al.(LHCb Collaboration), Observation of an exotic narrow doubly charmed tetraquark, Nat. Phys.18, 751 (2022)

  69. [69]

    Aaijet al.(LHCb Collaboration), Study of the doubly charmed tetraquarkT + cc, Nat

    R. Aaijet al.(LHCb Collaboration), Study of the doubly charmed tetraquarkT + cc, Nat. Commun.13, 3351 (2022)

  70. [70]

    A. V . Manohar and M. B. Wise, ExoticQQ¯q¯qstates in QCD, Nucl. Phys. B399, 17 (1993)

  71. [71]

    T. E. O. Ericson and G. Karl, Strength of pion exchange in hadronic molecules, Phys. Lett. B309, 426 (1993)

  72. [72]

    N. A. Tornqvist, From the deuteron to deusons, an analysis of deuteron-like meson-meson bound states, Z. Phys. C61, 525 (1994)

  73. [73]

    Janc and M

    D. Janc and M. Rosina, TheT cc =DD ∗ molecular state, Few- Body Syst.35, 175 (2004)

  74. [74]

    G. J. Ding, J. F. Liu, and M. L. Yan, Dynamics of Hadronic Molecule in One-Boson Exchange Approach and Possible Heavy Flavor Molecules, Phys. Rev. D79, 054005 (2009)

  75. [75]

    Molina, T

    R. Molina, T. Branz, and E. Oset, A new interpretation for the D∗ s2(2573) and the prediction of novel exotic charmed mesons, Phys. Rev. D82, 014010 (2010)

  76. [76]

    Ohkoda, Y

    S. Ohkoda, Y . Yamaguchi, S. Yasui, K. Sudoh, and A. Hosaka, Exotic mesons with double charm and bottom flavor, Phys. Rev. D86, 034019 (2012)

  77. [77]

    N. Li, Z. F. Sun, X. Liu, and S. L. Zhu, Coupled-channel anal- ysis of The possibleD (∗)D(∗), ¯B(∗) ¯B(∗) andD (∗) ¯B(∗) molecular states, Phys. Rev. D88, 114008 (2013)

  78. [78]

    H. Xu, B. Wang, Z. W. Liu, and X. Liu,DD ∗ potentials in chiral perturbation theory and possible molecular states, Phys. Rev. D99, 014027 (2019)

  79. [79]

    M. Z. Liu, T. W. Wu, M. Pavon Valderrama, J. J. Xie, and L. S. Geng, Heavy-quark spin and flavor symmetry partners of theX(3872) revisited: What can we learn from the one boson 12 exchange model?, Phys. Rev. D99, 094018 (2019)

  80. [80]

    Z. M. Ding, H. Y . Jiang, and J. He, Molecular states from D(∗) ¯D(∗)/B(∗) ¯B(∗) andD (∗)D(∗)/ ¯B(∗) ¯B(∗) interactions, Eur. Phys. J. C80, 1179 (2020)

Showing first 80 references.