Muonic Boson Limits: Supernova Redux
arXiv:2109.03244 · doi:10.1103/PhysRevD.105.035022
Abstract
We derive supernova (SN) bounds on muon-philic bosons, taking advantage of the recent emergence of muonic SN models. Our main innovations are to consider scalars in addition to pseudoscalars and to include systematically the generic two-photon coupling implied by a muon triangle loop. This interaction allows for Primakoff scattering and radiative boson decays. The globular-cluster bound derived for axion-like particles carries over to the muonic Yukawa couplings as and for keV, so SN arguments become interesting mainly for larger masses. If bosons escape freely from the SN core the main constraints originate from SN1987A rays and the diffuse cosmic -ray background. The latter allows at most of a typical total SN energy of erg to show up as rays, for keV implying and . In the trapping regime the bosons emerge as quasi-thermal radiation from a region near the neutrino sphere and match for . However, the decay is so fast that all the energy is dumped into the surrounding progenitor-star matter, whereas at most may show up in the explosion. To suppress boson emission below this level we need yet larger couplings, and . Muonic scalars can explain the muon magnetic-moment anomaly for , a value hard to reconcile with SN physics despite the uncertainty of the explosion-energy bound. For generic axion-like particles, this argument covers the "cosmological triangle" in the -- parameter space.
30 pages, 12 figures; v3 typographical corrections (see Note Added) after publication
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