If dark matter interacts too strongly with nuclei, it could be slowed to undetectable speeds in Earth's crust or atmosphere before ever reaching a detector. For sub-GeV dark matter, analytic approximations appropriate for heavier dark matter fail, necessitating the use of computationally expensive simulations. We present a new method of modeling attenuation of light dark matter in the Earth, based on the approximation that the scattering is isotropic in the lab frame. We show that this approach agrees well with Monte Carlo results, and can be much faster when the number of scatterings becomes large, as the runtime for Monte Carlo methods increases exponentially with cross section. We use this method to model attenuation for sub-dominant dar...
In the thermal dark matter (DM) paradigm, primordial interactions between DM and Standard Model part...
Direct detection experiments utilizing electronic excitations are spearheading the search for light,...
Dark matter (DM) can be captured in celestial bodies after scattering and losing sufficient energy t...
The scattering of light dark matter off thermal electrons inside the Sun produces a "fast" sub-compo...
The irreducible upscattering of cold dark matter by cosmic rays opens up the intriguing possibility ...
We emphasize the distinctive cosmological dynamics in multi-component dark matter scenarios and its ...
Dark Matter experiments searching for Weakly interacting massive particles (WIMPs) primarily use nuc...
The null signal from collider and dark matter (DM) direct detector experiments makes the interaction...
Direct detection for sub-GeV dark matter is developing rapidly, with many novel experimental ideas a...
We consider a dark sector scenario with two dark matter species with opposite dark $U(1)$ charges an...
Optically dense clouds in the interstellar medium composed predominantly of molecular hydrogen, know...
We show that dark-matter candidates with large masses and large nuclear interaction cross sections a...
Dark matters with MeV- or keV-scale mass are difficult to detect with standard direct search detecto...
Journal ArticleWe present two examples of velocity distributions for light dark matter particles tha...
We study the probing prospects of cosmic ray boosted dark matter (DM) in the framework of electron-p...
In the thermal dark matter (DM) paradigm, primordial interactions between DM and Standard Model part...
Direct detection experiments utilizing electronic excitations are spearheading the search for light,...
Dark matter (DM) can be captured in celestial bodies after scattering and losing sufficient energy t...
The scattering of light dark matter off thermal electrons inside the Sun produces a "fast" sub-compo...
The irreducible upscattering of cold dark matter by cosmic rays opens up the intriguing possibility ...
We emphasize the distinctive cosmological dynamics in multi-component dark matter scenarios and its ...
Dark Matter experiments searching for Weakly interacting massive particles (WIMPs) primarily use nuc...
The null signal from collider and dark matter (DM) direct detector experiments makes the interaction...
Direct detection for sub-GeV dark matter is developing rapidly, with many novel experimental ideas a...
We consider a dark sector scenario with two dark matter species with opposite dark $U(1)$ charges an...
Optically dense clouds in the interstellar medium composed predominantly of molecular hydrogen, know...
We show that dark-matter candidates with large masses and large nuclear interaction cross sections a...
Dark matters with MeV- or keV-scale mass are difficult to detect with standard direct search detecto...
Journal ArticleWe present two examples of velocity distributions for light dark matter particles tha...
We study the probing prospects of cosmic ray boosted dark matter (DM) in the framework of electron-p...
In the thermal dark matter (DM) paradigm, primordial interactions between DM and Standard Model part...
Direct detection experiments utilizing electronic excitations are spearheading the search for light,...
Dark matter (DM) can be captured in celestial bodies after scattering and losing sufficient energy t...