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Axions constituting dark matter (DM) are often considered to form a non-relativistic oscillating field. We explore bursts of relativistic axions from transient astrophysical sources, such as axion star explosions, where the sources are initially non-relativistic. For the QCD axion, bursts from collapsing axion stars lead to potentially detectable signals over a wide range of axion masses $10^{-15} , textrm{eV} lesssim m lesssim 10^{-7} , textrm{eV}$ in future experiments, such as ABRACADABRA, DMRadio and SHAFT. Unlike conventional cold axion DM searches, the sensitivity to axion bursts is not necessarily suppressed as $1/f$ for large decay constants $f$. The detection of axion bursts could provide new insights into the fundamental axion potential, which is challenging to probe otherwise. An ensemble of bursts in the distant past, in direct analogy with neutrinos, would give rise to a diffuse axion background distinct from the usual cold axion DM. Coincidence with other signatures, such as electromagnetic and gravitational-wave emission, would provide a new beyond-the-standard-model window into multi-messenger astronomy.
Time domain astronomy has come of age with astronomers now able to monitor the sky at high cadence both across the electromagnetic spectrum and using neutrinos and gravitational waves. The advent of new observing facilities permits new science, but t
The physics case for axions and axion-like particles is reviewed and an overview of ongoing and near-future laboratory searches is presented.
We propose a class of axion models with generation dependent Peccei-Quinn charges for the known fermions that allow to suppress the axion couplings to nucleons and electrons. Astrophysical limits are thus relaxed, allowing for axion masses up to ${ca
We examine the cosmological and astrophysical signatures of a dark baryon, a neutral fermion that mixes with the neutron. As the mixing is through a higher-dimensional operator at the quark level, production of the dark baryon at high energies is enh
We study the dynamics of the Peccei-Quinn (PQ) phase transition for the QCD axion. In weakly coupled models the transition is typically second order except in the region of parameters where the PQ symmetry is broken through the Coleman-Weinberg mecha