A sensitivity forecast shows H.E.S.S.-like, CTAO, and SWGO observations could strengthen ALP-photon coupling limits by about an order of magnitude over gamma-ray satellites and probe axion-electron couplings at lower masses.
Inverse Primakoff Scattering for Axionlike Particle Coupling
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
Axionlike particles (ALPs) can be produced in the Sun, and are considered viable candidates for the cosmological dark matter (DM). It can decay into two photons or interact with matter. We identify new inelastic channels of inverse Primakoff processes due to atomic excitation and ionization. Their cross sections are derived by incorporating full electromagnetic fields of atomic charge and current densities, and computed by well-benchmarked atomic many-body methods. Complementing data from the underground XENONnT and surface TEXONO experiments are analyzed. Event rates and sensitivity reaches are evaluated with respect to solar- and DM-ALPs. New parameter space in ALP couplings with the photons versus ALP masses in (1~eV$-$10~keV) not previously accessible to laboratory experiments are probed and excluded with solar-ALPs. However, at regions where DM-ALPs have already decayed, there would be no ALP-flux and hence no interactions at the detectors in direct search experiments. No physics constraints can be derived. Future projects would be able to evade the stability bound and open new observable windows in (100~eV$-$1~MeV) for DM-ALPs.
citation-role summary
citation-polarity summary
fields
astro-ph.HE 1years
2025 1verdicts
CONDITIONAL 1roles
background 1polarities
background 1representative citing papers
citing papers explorer
-
Probing axion-like particles through the gamma-ray production from cosmic-ray scattering in the Milky Way dark matter halo
A sensitivity forecast shows H.E.S.S.-like, CTAO, and SWGO observations could strengthen ALP-photon coupling limits by about an order of magnitude over gamma-ray satellites and probe axion-electron couplings at lower masses.