Incoherent fermionic dark matter absorption with nucleon Fermi motion

We investigate the incoherent regime of the fermionic dark matter absorption by nuclei using the relativistic Fermi gas model and nuclear form factors. With the momentum transfer being roughly equal to the dark matter mass <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:msub><a:mi>m</a:mi><a:mi>χ</a:mi></a:msub></a:math>, the incoherent regime contributes significantly to the absorption process for <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msub><c:mi>m</c:mi><c:mi>χ</c:mi></c:msub><c:mo>≳</c:mo><c:mn>100</c:mn><c:mtext> </c:mtext><c:mtext> </c:mtext><c:mi>MeV</c:mi></c:math> with a spin-independent operator and for even smaller mass with a spin-dependent one. We also compare the situations for various target nuclei (<e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mrow><e:mmultiscripts><e:mrow><e:mi>Xe</e:mi></e:mrow><e:mprescripts/><e:none/><e:mrow><e:mn>131</e:mn></e:mrow></e:mmultiscripts></e:mrow></e:math>, <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mrow><g:mmultiscripts><g:mrow><g:mi>Ge</g:mi></g:mrow><g:mprescripts/><g:none/><g:mrow><g:mn>72</g:mn></g:mrow></g:mmultiscripts></g:mrow></g:math>, <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:mrow><i:mmultiscripts><i:mrow><i:mi>Ar</i:mi></i:mrow><i:mprescripts/><i:none/><i:mrow><i:mn>40</i:mn></i:mrow></i:mmultiscripts></i:mrow></i:math>, <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mrow><k:mmultiscripts><k:mrow><k:mi>Ne</k:mi></k:mrow><k:mprescripts/><k:none/><k:mrow><k:mn>20</k:mn></k:mrow></k:mmultiscripts></k:mrow></k:math>, and <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mrow><m:mmultiscripts><m:mrow><m:mi>He</m:mi></m:mrow><m:mprescripts/><m:none/><m:mrow><m:mn>4</m:mn></m:mrow></m:mmultiscripts></m:mrow></m:math>) that are typically used in the dark matter direct detection. A heavier nucleus actually has the advantage of probing the incoherent scattering of the fermionic absorption dark matter. Observing both the coherent and incoherent contributions would be an important justification of the fermionic dark matter absorption. Published by the American Physical Society 2024

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Journal
Physical review. D/Physical review. D.
Published
2024-09-03
DOI
https://doi.org/10.1103/physrevd.110.055003
Citations
4
Primary Topic
Dark Matter and Cosmic Phenomena
Type
article
Field-Weighted Citation Impact
2.64

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article

Incoherent fermionic dark matter absorption with nucleon Fermi motion

O. A. Titov, Shao-Feng Ge
4 citations
Physical review. D/Physical review. D.
Dark Matter and Cosmic Phenomena
2.64
article

Incoherent fermionic dark matter absorption with nucleon Fermi motion

O. A. Titov, Shao-Feng Ge
article en
4 citations

Abstract

We investigate the incoherent regime of the fermionic dark matter absorption by nuclei using the relativistic Fermi gas model and nuclear form factors. With the momentum transfer being roughly equal to the dark matter mass <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:msub><a:mi>m</a:mi><a:mi>χ</a:mi></a:msub></a:math>, the incoherent regime contributes significantly to the absorption process for <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msub><c:mi>m</c:mi><c:mi>χ</c:mi></c:msub><c:mo>≳</c:mo><c:mn>100</c:mn><c:mtext> </c:mtext><c:mtext> </c:mtext><c:mi>MeV</c:mi></c:math> with a spin-independent operator and for even smaller mass with a spin-dependent one. We also compare the situations for various target nuclei (<e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mrow><e:mmultiscripts><e:mrow><e:mi>Xe</e:mi></e:mrow><e:mprescripts/><e:none/><e:mrow><e:mn>131</e:mn></e:mrow></e:mmultiscripts></e:mrow></e:math>, <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mrow><g:mmultiscripts><g:mrow><g:mi>Ge</g:mi></g:mrow><g:mprescripts/><g:none/><g:mrow><g:mn>72</g:mn></g:mrow></g:mmultiscripts></g:mrow></g:math>, <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:mrow><i:mmultiscripts><i:mrow><i:mi>Ar</i:mi></i:mrow><i:mprescripts/><i:none/><i:mrow><i:mn>40</i:mn></i:mrow></i:mmultiscripts></i:mrow></i:math>, <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mrow><k:mmultiscripts><k:mrow><k:mi>Ne</k:mi></k:mrow><k:mprescripts/><k:none/><k:mrow><k:mn>20</k:mn></k:mrow></k:mmultiscripts></k:mrow></k:math>, and <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mrow><m:mmultiscripts><m:mrow><m:mi>He</m:mi></m:mrow><m:mprescripts/><m:none/><m:mrow><m:mn>4</m:mn></m:mrow></m:mmultiscripts></m:mrow></m:math>) that are typically used in the dark matter direct detection. A heavier nucleus actually has the advantage of probing the incoherent scattering of the fermionic absorption dark matter. Observing both the coherent and incoherent contributions would be an important justification of the fermionic dark matter absorption. Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(5)
Shanghai Jiao Tong University (CN)
National Natural Science Foundation of China, Shanghai Jiao Tong University
Openalex Percentile: Top 7%
Dark Matter and Cosmic Phenomena
2.64
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