Aspects of a Five-Dimensional $U(1)_{L_\mu - L_\tau}$ Model at Future Muon-Based Colliders

TL;DR

This paper investigates a five-dimensional U(1)_{L_mu-L_tau} gauge model with Kaluza-Klein excitations, analyzing how future muon colliders can probe its parameter space beyond current experimental limits.

Contribution

It demonstrates that future muon-based colliders can effectively explore heavy and light KK gauge bosons in the model, extending the reach of low-energy experiments.

Findings

Future colliders can probe TeV-scale KK gauge bosons with large couplings.

They can also detect MeV-scale KK gauge bosons with very weak couplings.

The experiments could achieve a 2σ exclusion over a broad mass range.

Abstract

We study a five-dimensional (5D) framework based on the \(U(1)_{L_\mu-L_\tau}\) gauge symmetry, where the associated gauge field \(V\) propagates in the bulk, giving rise to an infinite tower of Kaluza--Klein (KK) excitations \(V^{(n)}\) that couple selectively to the second- and third-generation leptons. Originally motivated by its potential to address the muon \(g-2\) anomaly, this framework remains of interest as a minimal, anomaly-free, phenomenologically well-motivated extension of the Standard Model (SM) of particle physics. We focus on high-energy muon-based colliders, which could directly probe the gauge structure without relying on the kinetic mixing between the SM hypercharge gauge boson and the 5D gauge boson \(V\). We explore a set of complementary processes: the elastic $\mu^+\mu^+ \to \mu^+\mu^+$ scattering via off-shell exchange of KK (gauge) excitations \(V^{(n)}\); the bremsstrahlung production of \(V^{(n)}\) followed by their decays into neutrinos and into $\mu^-\mu^+$ at a future $\mu$TRISTAN collider. Further, we study the $\mu^-\mu^+ \to \mu^-\mu^+$ scattering via resonant KK excitation(s) at a future muon collider. Our results show that these future muon-based colliders could offer sensitive and complementary probes into regions in the parameter space of the scenario that are beyond the reach of low-energy experiments. In particular, such experiments would be able to probe both heavier such KK gauge bosons with TeV-scale masses for relatively large gauge couplings, as well as the much lighter ones with masses in the MeV-scale for couplings as weak as \(g_D \sim \mathcal{O}(10^{-5})\), thereby offering a promising $2\sigma$ exclusion reach for such KK excitations, over an extensive range of masses, at these facilities.