# Dark Photons from Captured Inelastic Dark Matter Annihilation: Charged Particle Signatures

## TL;DR

This paper explores how inelastic dark matter interactions via dark photons could produce detectable positron signals in AMS-02, relaxing direct detection constraints and identifying a viable parameter space for future searches.

## Contribution

It extends previous models by analyzing inelastic dark matter with nearly degenerate species, revealing a new parameter space where AMS-02 can detect signals despite existing constraints.

## Key findings

- Positron signals remain similar to elastic case for small mass splittings.
- Inelastic dark matter relaxes direct detection constraints.
- Viable parameter space identified for dark matter mass 100 GeV to 10 TeV, dark photon mass 1-100 MeV.

## Abstract

The dark sector may contain a dark photon that kinetically mixes with the Standard Model photon, allowing dark matter to interact weakly with normal matter. In previous work we analyzed the implications of this scenario for dark matter capture by the Sun. Dark matter will gather in the core of the Sun and annihilate to dark photons. These dark photons travel outwards from the center of the Sun and may decay to produce positrons that can be detected by the Alpha Magnetic Spectrometer (AMS-02) on the ISS. We found that the dark photon parameter space accessible to this analysis is largely constrained by strong limits on the spin-independent WIMP-nucleon cross section from direct detection experiments. In this paper we build upon previous work by considering the case where the dark sector contains two species of Dirac fermion that are nearly degenerate in mass and couple inelastically to the dark photon. We find that for small values of the mass splitting $\Delta \sim 100 ~\text{keV}$, the predicted positron signal at AMS-02 remains largely unchanged from the previously considered elastic case while constraints from direct detection are relaxed, leaving a region of parameter space with dark matter mass $100 ~\text{GeV} \lesssim m_X \lesssim 10 ~\text{TeV}$, dark photon mass $1 ~\text{MeV} \lesssim m_{A'} \lesssim 100 ~\text{MeV}$, and kinetic mixing parameter $10^{-9} \lesssim \varepsilon \lesssim 10^{-8}$ that is untouched by supernova observations and fixed target experiments but where an inelastic dark sector may still be discovered using existing AMS-02 data.