(In)direct detection of boosted dark matter

We initiate the study of novel thermal dark matter (DM) scenarios where present-day annihilation of DM in the galactic center produces boosted stable particles in the dark sector. These stable particles are typically a subdominant DM component, but because they are produced with a large Lorentz boos...

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Main Authors: Agashe, Kaustubh, Cui, Yanou, Necib, Lina, Thaler, Jesse
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics
Format: Article
Language:en_US
Published: IOP Publishing 2015
Online Access:http://hdl.handle.net/1721.1/98427
https://orcid.org/0000-0003-2806-1414
https://orcid.org/0000-0002-2406-8160
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author Agashe, Kaustubh
Cui, Yanou
Necib, Lina
Thaler, Jesse
author2 Massachusetts Institute of Technology. Center for Theoretical Physics
author_facet Massachusetts Institute of Technology. Center for Theoretical Physics
Agashe, Kaustubh
Cui, Yanou
Necib, Lina
Thaler, Jesse
author_sort Agashe, Kaustubh
collection MIT
description We initiate the study of novel thermal dark matter (DM) scenarios where present-day annihilation of DM in the galactic center produces boosted stable particles in the dark sector. These stable particles are typically a subdominant DM component, but because they are produced with a large Lorentz boost in this process, they can be detected in large volume terrestrial experiments via neutral-current-like interactions with electrons or nuclei. This novel DM signal thus combines the production mechanism associated with indirect detection experiments (i.e. galactic DM annihilation) with the detection mechanism associated with direct detection experiments (i.e. DM scattering off terrestrial targets). Such processes are generically present in multi-component DM scenarios or those with non-minimal DM stabilization symmetries. As a proof of concept, we present a model of two-component thermal relic DM, where the dominant heavy DM species has no tree-level interactions with the standard model and thus largely evades direct and indirect DM bounds. Instead, its thermal relic abundance is set by annihilation into a subdominant lighter DM species, and the latter can be detected in the boosted channel via the same annihilation process occurring today. Especially for dark sector masses in the 10 MeV–10 GeV range, the most promising signals are electron scattering events pointing toward the galactic center. These can be detected in experiments designed for neutrino physics or proton decay, in particular Super-K and its upgrade Hyper-K, as well as the PINGU/MICA extensions of IceCube. This boosted DM phenomenon highlights the distinctive signatures possible from non-minimal dark sectors.
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spelling mit-1721.1/984272022-09-30T13:57:39Z (In)direct detection of boosted dark matter Agashe, Kaustubh Cui, Yanou Necib, Lina Thaler, Jesse Massachusetts Institute of Technology. Center for Theoretical Physics Massachusetts Institute of Technology. Department of Physics Necib, Lina Thaler, Jesse We initiate the study of novel thermal dark matter (DM) scenarios where present-day annihilation of DM in the galactic center produces boosted stable particles in the dark sector. These stable particles are typically a subdominant DM component, but because they are produced with a large Lorentz boost in this process, they can be detected in large volume terrestrial experiments via neutral-current-like interactions with electrons or nuclei. This novel DM signal thus combines the production mechanism associated with indirect detection experiments (i.e. galactic DM annihilation) with the detection mechanism associated with direct detection experiments (i.e. DM scattering off terrestrial targets). Such processes are generically present in multi-component DM scenarios or those with non-minimal DM stabilization symmetries. As a proof of concept, we present a model of two-component thermal relic DM, where the dominant heavy DM species has no tree-level interactions with the standard model and thus largely evades direct and indirect DM bounds. Instead, its thermal relic abundance is set by annihilation into a subdominant lighter DM species, and the latter can be detected in the boosted channel via the same annihilation process occurring today. Especially for dark sector masses in the 10 MeV–10 GeV range, the most promising signals are electron scattering events pointing toward the galactic center. These can be detected in experiments designed for neutrino physics or proton decay, in particular Super-K and its upgrade Hyper-K, as well as the PINGU/MICA extensions of IceCube. This boosted DM phenomenon highlights the distinctive signatures possible from non-minimal dark sectors. United States. Dept. of Energy (Cooperative Research Agreement DE-FG02-05ER-41360) United States. Dept. of Energy (Early Career Research Program DE-FG02-11ER-41741) Alfred P. Sloan Foundation (Sloan Research Fellowship) 2015-09-10T12:28:48Z 2015-09-10T12:28:48Z 2014-10 2014-09 Article http://purl.org/eprint/type/JournalArticle 1475-7516 1475-7508 http://hdl.handle.net/1721.1/98427 Agashe, Kaustubh, Yanou Cui, Lina Necib, and Jesse Thaler. “(In)direct Detection of Boosted Dark Matter.” Journal of Cosmology and Astroparticle Physics 2014, no. 10 (October 1, 2014): 062–062. https://orcid.org/0000-0003-2806-1414 https://orcid.org/0000-0002-2406-8160 en_US http://dx.doi.org/10.1088/1475-7516/2014/10/062 Journal of Cosmology and Astroparticle Physics Creative Commons Attribution http://creativecommons.org/licenses/by/4.0/ application/pdf IOP Publishing IOP
spellingShingle Agashe, Kaustubh
Cui, Yanou
Necib, Lina
Thaler, Jesse
(In)direct detection of boosted dark matter
title (In)direct detection of boosted dark matter
title_full (In)direct detection of boosted dark matter
title_fullStr (In)direct detection of boosted dark matter
title_full_unstemmed (In)direct detection of boosted dark matter
title_short (In)direct detection of boosted dark matter
title_sort in direct detection of boosted dark matter
url http://hdl.handle.net/1721.1/98427
https://orcid.org/0000-0003-2806-1414
https://orcid.org/0000-0002-2406-8160
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