Dark sink enhances the direct detection of freeze-in dark matter

We describe a simple dark sector structure which, if present, has implications for the direct detection of dark matter (DM); . A dark sink transports energy density from the DM into light dark-sector states that do not appreciably contribute to the DM density. As an example, we consider a light, neutral fermion <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>ψ</a:mi></a:math> which interacts solely with DM <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>χ</c:mi></c:math> via the exchange of a heavy scalar <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi mathvariant="normal">Φ</e:mi></e:math>. We illustrate the impact of a dark sink by adding one to a DM freeze-in model in which <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mi>χ</h:mi></h:math> couples to a light dark photon <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:msup><j:mi>γ</j:mi><j:mo>′</j:mo></j:msup></j:math> which kinetically mixes with the Standard Model (SM) photon. This freeze-in model (absent the sink) is itself a benchmark for ongoing experiments. In some cases, the literature for this benchmark has contained errors; we correct the predictions and provide them as a public code. We then analyze how the dark sink modifies this benchmark, solving coupled Boltzmann equations for the dark-sector energy density and DM yield. We check the contribution of the dark sink <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"><l:mi>ψ</l:mi></l:math>’s to dark radiation; consistency with existing data limits the maximum attainable cross section. For DM with a mass between <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"><n:mi>MeV</n:mi><n:mo>−</n:mo><n:mi mathvariant="script">O</n:mi><n:mo stretchy="false">(</n:mo><n:mn>10</n:mn><n:mtext> </n:mtext><n:mtext> </n:mtext><n:mi>GeV</n:mi><n:mo stretchy="false">)</n:mo></n:math>, adding the dark sink can increase predictions for the direct detection cross section all the way up to the current limits. Published by the American Physical Society 2024

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2024-08-12
DOI
https://doi.org/10.1103/physrevd.110.l031702
Citations
22
Primary Topic
Dark Matter and Cosmic Phenomena
Type
article
Field-Weighted Citation Impact
14.51

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article

Dark sink enhances the direct detection of freeze-in dark matter

Aaron Pierce, Prudhvi N. Bhattiprolu, Robert McGehee
22 citations
Physical review. D/Physical review. D.
Dark Matter and Cosmic Phenomena
14.51
article

Dark sink enhances the direct detection of freeze-in dark matter

Aaron Pierce, Prudhvi N. Bhattiprolu, Robert McGehee
article en
22 citations

Abstract

We describe a simple dark sector structure which, if present, has implications for the direct detection of dark matter (DM); . A dark sink transports energy density from the DM into light dark-sector states that do not appreciably contribute to the DM density. As an example, we consider a light, neutral fermion <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>ψ</a:mi></a:math> which interacts solely with DM <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>χ</c:mi></c:math> via the exchange of a heavy scalar <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi mathvariant="normal">Φ</e:mi></e:math>. We illustrate the impact of a dark sink by adding one to a DM freeze-in model in which <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mi>χ</h:mi></h:math> couples to a light dark photon <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:msup><j:mi>γ</j:mi><j:mo>′</j:mo></j:msup></j:math> which kinetically mixes with the Standard Model (SM) photon. This freeze-in model (absent the sink) is itself a benchmark for ongoing experiments. In some cases, the literature for this benchmark has contained errors; we correct the predictions and provide them as a public code. We then analyze how the dark sink modifies this benchmark, solving coupled Boltzmann equations for the dark-sector energy density and DM yield. We check the contribution of the dark sink <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"><l:mi>ψ</l:mi></l:math>’s to dark radiation; consistency with existing data limits the maximum attainable cross section. For DM with a mass between <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"><n:mi>MeV</n:mi><n:mo>−</n:mo><n:mi mathvariant="script">O</n:mi><n:mo stretchy="false">(</n:mo><n:mn>10</n:mn><n:mtext> </n:mtext><n:mtext> </n:mtext><n:mi>GeV</n:mi><n:mo stretchy="false">)</n:mo></n:math>, adding the dark sink can increase predictions for the direct detection cross section all the way up to the current limits. Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(3)
University of Minnesota (US), University of Michigan (US), University of Minnesota System (US)
U.S. Department of Energy, Mainz Institute for Theoretical Physics, Johannes Gutenberg University Mainz
Affordable and clean energy
Openalex Percentile: Top 1%
Dark Matter and Cosmic Phenomena
14.51
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