[2025-01-18] For better promotion of the events, the categories in this system will be adjusted. For details, please refer to the announcement of this system. The link is https://indico-tdli.sjtu.edu.cn/news/1-warm-reminder-on-adjusting-indico-tdli-categories-indico
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This figure shows the truth-level recoil-electron energy and angular distributions for different sterile-neutrino masses. The recoil electron is mainly concentrated at low energy, indicating that most of the beam energy is carried away by invisible particles. As mNm_NmN increases, the angular distribution becomes broader, showing stronger kinematic effects from the heavier sterile neutrino.

This figure compares the reconstructed recoil-electron momentum of the sterile-neutrino signal with a dark-photon reference sample. The sterile-neutrino signal is generally softer, especially for lighter masses, meaning that the visible electron carries less momentum while the invisible final state carries away most of the beam energy.

This figure shows the reconstructed missing-momentum distribution. For light sterile neutrinos, the signal is concentrated at large missing momentum, which is a typical missing-energy signature. As mNm_NmN increases, the distribution shifts because the heavier invisible particle changes the event kinematics. This variable is therefore useful for defining and optimizing the signal region.

This figure shows the detector-level ECAL and HCAL energy distributions. Most signal events have very small HCAL energy, consistent with a final state containing a recoil electron and invisible particles but little hadronic activity. This supports the use of an HCAL veto and ECAL-based selection for the signal region.