Constraints on Sterile Neutrino Models from Strong Gravitational Lensing, Milky Way Satellites, and the Lyman-α Forest

Ioana A. Zelko (Department of Physics and Astronomy, University of California, Los Angeles, 475 Portola Plaza, Los Angeles, California 90095, USA) ; Tommaso Treu (Department of Physics and Astronomy, University of California, Los Angeles, 475 Portola Plaza, Los Angeles, California 90095, USA) ; Kevork N. Abazajian (Department of Physics and Astronomy, University of California, Irvine, Irvine, California 92697, USA) ; Daniel Gilman (Department of Astronomy and Astrophysics, University of Toronto, 50 St. George Street, Toronto, Ontario, M5S 3H4, Canada) ; Andrew J. Benson (Observatories of the Carnegie Institution for Science, 813 Santa Barbara Street, Pasadena, California 91101, USA) ; et al. - Show all 8 authors

The nature of dark matter is one of the most important unsolved questions in science. Some dark matter candidates do not have sufficient nongravitational interactions to be probed in laboratory or accelerator experiments. It is thus important to develop astrophysical probes which can constrain or lead to a discovery of such candidates. We illustrate this using state-of-the-art measurements of strong gravitationally lensed quasars to constrain four of the most popular sterile neutrino models, and also report the constraints for other independent methods that are comparable in procedure. First, we derive effective relations to describe the correspondence between the mass of a thermal relic warm dark matter particle and the mass of sterile neutrinos produced via Higgs decay and grand unified theory (GUT)-scale scenarios, in terms of large-scale structure and galaxy formation astrophysical effects. Second, we show that sterile neutrinos produced through the Higgs decay mechanism are allowed only for mass >26 keV, and GUT-scale scenario >5.3 keV. Third, we show that the single sterile neutrino model produced through active neutrino oscillations is allowed for mass >92 keV, and the three sterile neutrino minimal standard model (νMSM) for mass >16 keV. These are the most stringent experimental limits on these models.

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      "source": "APS", 
      "value": "The nature of dark matter is one of the most important unsolved questions in science. Some dark matter candidates do not have sufficient nongravitational interactions to be probed in laboratory or accelerator experiments. It is thus important to develop astrophysical probes which can constrain or lead to a discovery of such candidates. We illustrate this using state-of-the-art measurements of strong gravitationally lensed quasars to constrain four of the most popular sterile neutrino models, and also report the constraints for other independent methods that are comparable in procedure. First, we derive effective relations to describe the correspondence between the mass of a thermal relic warm dark matter particle and the mass of sterile neutrinos produced via Higgs decay and grand unified theory (GUT)-scale scenarios, in terms of large-scale structure and galaxy formation astrophysical effects. Second, we show that sterile neutrinos produced through the Higgs decay mechanism are allowed only for mass <math><mo>&gt;</mo><mn>26</mn><mtext> </mtext><mtext> </mtext><mi>keV</mi></math>, and GUT-scale scenario <math><mo>&gt;</mo><mn>5.3</mn><mtext> </mtext><mtext> </mtext><mi>keV</mi></math>. Third, we show that the single sterile neutrino model produced through active neutrino oscillations is allowed for mass <math><mo>&gt;</mo><mn>92</mn><mtext> </mtext><mtext> </mtext><mi>keV</mi></math>, and the three sterile neutrino minimal standard model (<math><mrow><mi>\u03bd</mi><mi>MSM</mi></mrow></math>) for mass <math><mo>&gt;</mo><mn>16</mn><mtext> </mtext><mtext> </mtext><mi>keV</mi></math>. These are the most stringent experimental limits on these models."
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Published on:
04 November 2022
Publisher:
APS
Published in:
Physical Review Letters , Volume 129 (2022)
Issue 19
DOI:
https://doi.org/10.1103/PhysRevLett.129.191301
arXiv:
2205.09777
Copyrights:
Published by the American Physical Society
Licence:
CC-BY-4.0

Fulltext files: