English

Simulating Heavy Neutral Leptons with General Couplings at Collider and Fixed Target Experiments

High Energy Physics - Phenomenology 2024-06-10 v2 High Energy Physics - Experiment

Abstract

Heavy neutral leptons (HNLs) are motivated by attempts to explain neutrino masses and dark matter. If their masses are in the MeV to several GeV range, HNLs are light enough to be copiously produced at collider and accelerator facilities, but also heavy enough to decay to visible particles on length scales that can be observed in particle detectors. Previous studies evaluating the sensitivities of experiments have often focused on simple, but not particularly well-motivated, models in which the HNL mixes with only one active neutrino flavor. In this work, we accurately simulate models for HNL masses between 100 MeV and 10 GeV and arbitrary couplings to ee, μ\mu, and τ\tau leptons. We include over 150 HNL production channels and over 100 HNL decay modes, including all of the processes that can be dominant in some region of the general parameter space. The result is HNLCalc, a user-friendly, fast, and flexible library to compute the properties of HNL models. As examples, we implement HNLCalc to extend the FORESEE package to evaluate the prospects for HNL discovery at forward LHC experiments. We present sensitivity reaches for FASER and FASER2 in five benchmark scenarios with coupling ratios Ue2:Uμ2:Uτ2|U_e|^2 : |U_\mu|^2 : |U_{\tau}|^2 = 1:0:0, 0:1:0, 0:0:1, 0:1:1, and 1:1:1, where the latter two have not been studied previously. Comparing these to current constraints, we identify regions of parameter space with significant discovery prospects.

Keywords

Cite

@article{arxiv.2405.07330,
  title  = {Simulating Heavy Neutral Leptons with General Couplings at Collider and Fixed Target Experiments},
  author = {Jonathan L. Feng and Alec Hewitt and Felix Kling and Daniel La Rocco},
  journal= {arXiv preprint arXiv:2405.07330},
  year   = {2024}
}

Comments

22 pages, 10 figures; v2: added references

R2 v1 2026-06-28T16:24:40.593Z