Searching for axion-like particles from tau exotic decays at the Super Tau-Charm Facility and its far detectors
Xu-Hui Jiang, Chih-Ting Lu
TL;DR
The paper investigates leptophilic axion-like particles (ALPs) produced in exotic tau decays at the future Super Tau-Charm Facility (STCF). It develops an effective field theory framework for ALP–lepton interactions, examining two electroweak structures (EW preserving and EW violating) and two decay scenarios (tauphilic and LFU), and analyzes both prompt and far-detector strategies to maximize reach. Using Monte Carlo simulations, it derives sensitivities across ALP masses and couplings, showing that tauphilic ALPs can be probed in a high-mass region around $m_a\sim 1$ GeV with lifetimes enabling far-detector detection, while LFU ALPs yield much shorter lifetimes, enhancing main-detector searches in the $m_a \sim 100$–$200$ MeV range. The results demonstrate the STCF’s potential to explore previously unprobed regions of leptophilic ALP parameter space and motivate the development of a far detector to complement the main detector.
Abstract
Leptophilic axion-like particles (ALPs) extend the Standard Model (SM) with brand-new interactions between the ALP and leptons. In this work, we focus on studying exotic $τ$ decays to explore such ALPs. Both the tauphilic and lepton flavor universal (LFU) scenarios, with electroweak preserving and violating benchmarks, have been investigated at a future $τ$-factory, namely the Super Tau-Charm Facility (STCF) under development in China. Both prompt and far detection are proposed, targeting on leptonic $τ$ decays, $τ^- \to \ell^-\barν_\ell ν_τa$. For prompt detection, the $τ^+τ^-$ threshold $\sqrt s=3.56$ GeV and higher central energy $\sqrt s=4.2$ GeV are taken into account. In addition, a cylinder-like far detector has been proposed to complement prompt detection. We demonstrate the huge potential to detect leptophilic ALPs at the STCF. Concretely, for tauphilic scenario, the STCF is mostly sensitive in the currently unprobed region with $m_a\sim 1000$ MeV. However, in the LFU scenario, the dilepton channel tremendously shortens the ALP lifetime, and eventually the STCF only allows a precise measurement in the new regime with $100~\text{MeV}\lesssim m_a\lesssim 200~\text{MeV}$.
