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Decoding Zc(4430) and Zc(4200): The role of P-wave charmed mesons

Jian-Bo Cheng1,2,*, Zi-Yang Lin2,†, Jun-Zhang Wang3,‡, and Shi-Lin Zhu2,§

  • *Contact author: jbcheng@pku.edu.cn
  • †Contact author: lzy_15@pku.edu.cn
  • ‡Contact author: wangjzh@cqu.edu.cn
  • §Contact author: zhusl@pku.edu.cn

Phys. Rev. D 113, 096001 – Published 5 May, 2026

DOI: https://doi.org/10.1103/v5jm-59g9

Abstract

In this work, we perform a systematic investigation of the hidden-charm tetraquark states with IG(JPC)=1+(1+−) within the hadronic molecular picture, placing particular emphasis on systems composed of an S-wave (D,D*) meson and a P-wave [D0*(2300),D1(2430),D1(2420),D2*(2460)] meson. Adopting the one-boson exchange potential, we solve the Schrödinger equation in momentum space via the complex scaling method. A crucial feature of our approach is the rigorous treatment of the unstable nature of the P-wave constituents by incorporating three-body decay effects arising from self-energy corrections and the static limit approximation. Our results demonstrate that these three-body dynamics play a crucial role in determining the pole positions, specifically in reproducing the large decay widths observed experimentally. We identify several broad resonances in the D*D¯1(2420) and D*D¯2*(2460) systems as candidates for the Zc(4430), while the significantly broader resonances in the DD¯0*(2300) and DD¯1(2430) sectors are suggested as candidates for the Zc(4200). Focusing on the D*D¯2*(2460) assignment as a specific case study, we further analyze the line shape of the Zc(4430) candidate using a Flatté-like parametrization with energy-dependent self-energy terms, providing predictions for its open-charm decay modes to guide future experimental searches.

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