Locate the mass at which the sideband constraint becomes ineffective
Determine the higgsino mass at which the high-energy sideband test ceases to impose a significant constraint on non-thermally produced higgsinos explaining the LZ event.
References
The $500$\,GeV benchmark is much less constrained by this, and we have not solved for the mass at which the transition occurs.
— Confronting the Higgsino Interpretation of the LZ Event with the High-Energy Sideband
(2609.04175 - Rodd et al., 3 Sep 2026) in Appendix A: Higgsinos away from the thermal mass