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Finite-temperature effects on the threshold cusps in ππ and DD¯* scatterings from relativistic heavy-ion collisions

Ying Zhang1,2,3,4,*, Atsushi Hosaka2,5,†, Qian Wang1,2,3,6,‡, and Shigehiro Yasui7,8,9,§

  • 1State Key Laboratory of Nuclear Physics and Technology, Institute of Quantum Matter, South China Normal University, Guangzhou 510006, China
  • 2Research Center for Nuclear Physics (RCNP), Osaka University, Ibaraki 567-0047, Japan
  • 3Key Laboratory of Atomic and Subatomic Structure and Quantum Control (MOE), Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Guangzhou 510006, China
  • 4Guangdong Basic Research Center of Excellence for Structure and Fundamental Interactions of Matter, Guangdong Provincial Key Laboratory of Nuclear Science, Guangzhou 510006, China
  • 5Advanced Science Research Center, Japan Atomic Energy Agency (JAEA), Tokai 319-1195, Japan
  • 6Southern Center for Nuclear-Science Theory (SCNT), Institute of Modern Physics, Chinese Academy of Sciences, Huizhou 516000, Guangdong Province, China
  • 7Nishogakusha University, 6-16, Sanbancho, Chiyoda, Tokyo 102-8336, Japan
  • 8Research and Education Center for Natural Sciences, Keio University, Hiyoshi 4-1-1, Yokohama, Kanagawa 223-8521, Japan
  • 9International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, 1-3-2 Kagamiyama, Higashi-Hiroshima, Hiroshima 739-8511, Japan

  • *Contact author: yingzhang@m.scnu.edu.cn, ying@rcnp.osaka-u.ac.jp
  • †Contact author: hosaka@rcnp.osaka-u.ac.jp
  • ‡Contact author: qianwang@m.scnu.edu.cn
  • §Contact author: yasuis@keio.jp

Phys. Rev. C 114, 015201 – Published 6 July, 2026

DOI: https://doi.org/10.1103/qxzl-rzz1

Abstract

We investigate how the temperature influences the threshold cusps in meson-meson scatterings, i.e., ππ and DD¯* (or D*D¯) scatterings, using the production rates and propagators obtained at finite temperature. The line shape of production rate of ππ at different temperatures demonstrates that the cusp structure in ππ scattering is mildly enhanced as the temperature increases. For the ππ propagator, which includes isospin symmetry breaking, the line shape displays a unique plateaulike structure, and this structure will also be enhanced as the temperature increases. For comparison, the line shape of the DD¯* propagator including isospin symmetry breaking is also investigated at different temperatures. As the temperature increases, its line shape shows a similar plateaulike structure but with some different properties when the temperature modifications to the masses and widths of D and D¯* are considered.

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