English

Probing hyperon electric dipole moments with a full angular analysis

High Energy Physics - Experiment 2023-12-29 v3

Abstract

The electric dipole moment (EDM) of elementary particles, arising from flavor-diagonal CPCP violation, serves as a powerful probe for new physics beyond the Standard Model and holds the potential to provide novel insights in unraveling the puzzle of the matter-dominated Universe. Hyperon EDM is a largely unexplored territory. In this paper, we present a comprehensive angular analysis that focuses on entangled hyperon-antihyperon pairs in J/ψJ/\psi decays for the indirect extraction of hyperon EDM. The statistical sensitivities are investigated for BESIII and the proposed Super Tau-Charm Facility (STCF). Leveraging the statistics from the BESIII experiment, the estimated sensitivity for Λ\Lambda EDM can reach an impressive level of 101910^{-19} ee cm, achieving a 3-orders-of-magnitude improvement over the only existing measurement in a fixed-target experiment at Fermilab with similar statistics. The estimated sensitivities for the Σ+\Sigma^+, Ξ\Xi^-, and Ξ0\Xi^0 hyperons at the same level of 101910^{-19} ee cm will mark the first-ever achievement and the latter two will be the first exploration of hyperons with two strange valence quarks. The EDM measurements for hyperons conducted at the BESIII experiment will be a significant milestone and serve as a litmus test for new physics such as supersymmetry and the left-right symmetrical model. Furthermore, at the STCF experiment, the sensitivity of hyperon EDM measurements can be further enhanced by 2 orders of magnitude. Additionally, this angular analysis enables the determination of CPCP violation in hyperon decays, the effective weak mixing angle, and beam polarization.

Keywords

Cite

@article{arxiv.2307.04364,
  title  = {Probing hyperon electric dipole moments with a full angular analysis},
  author = {Jinlin Fu and Hai-Bo Li and Jian-Peng Wang and Fu-Sheng Yu and Jianyu Zhang},
  journal= {arXiv preprint arXiv:2307.04364},
  year   = {2023}
}
R2 v1 2026-06-28T11:25:41.346Z