Deepest sensitivity to wavelike dark photon dark matter with superconducting radio frequency cavities

Wavelike, bosonic dark matter candidates like axions and dark photons can be detected using microwave cavities known as haloscopes. Traditionally, haloscopes consist of tunable copper cavities operating in the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:msub><a:mrow><a:mi>TM</a:mi></a:mrow><a:mrow><a:mn>010</a:mn></a:mrow></a:msub></a:mrow></a:math> mode, but ohmic losses have limited their performance. In contrast, superconducting radio frequency (SRF) cavities can achieve quality factors of <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mrow><c:mo>∼</c:mo><c:msup><c:mrow><c:mn>10</c:mn></c:mrow><c:mrow><c:mn>10</c:mn></c:mrow></c:msup></c:mrow></c:math>, perhaps 5 orders of magnitude better than copper cavities, leading to more sensitive dark matter detectors. In this paper, we first derive that the scan rate of a haloscope experiment is proportional to the loaded quality factor <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mrow><e:msub><e:mrow><e:mi>Q</e:mi></e:mrow><e:mrow><e:mi mathvariant="normal">L</e:mi></e:mrow></e:msub></e:mrow></e:math>, even if the cavity bandwidth is much narrower than the dark matter halo line shape. We then present a proof-of-concept search for dark photon dark matter using a nontunable ultrahigh-quality SRF cavity. We exclude dark photon dark matter with kinetic mixing strengths of <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mrow><h:mi>χ</h:mi><h:mo>&gt;</h:mo><h:mn>1.5</h:mn><h:mo>×</h:mo><h:msup><h:mrow><h:mn>10</h:mn></h:mrow><h:mrow><h:mo>−</h:mo><h:mn>16</h:mn></h:mrow></h:msup></h:mrow></h:math> for a dark photon mass of <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:mrow><j:msub><j:mrow><j:mi>m</j:mi></j:mrow><j:mrow><j:msup><j:mrow><j:mi>A</j:mi></j:mrow><j:mrow><j:mo>′</j:mo></j:mrow></j:msup></j:mrow></j:msub><j:mo>=</j:mo><j:mn>5.35</j:mn><j:mtext> </j:mtext><j:mtext> </j:mtext><j:mrow><j:mi mathvariant="normal">μ</j:mi><j:mi>eV</j:mi></j:mrow></j:mrow></j:math>, achieving the deepest exclusion to wavelike dark photons by almost an order of magnitude. 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.110.043022
Citations
13
Primary Topic
Dark Matter and Cosmic Phenomena
Type
article
Field-Weighted Citation Impact
8.58

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article

Deepest sensitivity to wavelike dark photon dark matter with superconducting radio frequency cavities

Sam Posen, R. Cervantes, D. Frolov, José Aumentado et al.
13 citations
Physical review. D/Physical review. D.
Dark Matter and Cosmic Phenomena
8.58
article

Deepest sensitivity to wavelike dark photon dark matter with superconducting radio frequency cavities

Sam Posen, R. Cervantes, D. Frolov, José Aumentado, Florent Lecocq, Alexander Romanenko, Bianca Giaccone, C. Braggio, Roni Harnik, Oleksandr Melnychuk, A. Grassellino, R. Pilipenko
article en
13 citations

Abstract

Wavelike, bosonic dark matter candidates like axions and dark photons can be detected using microwave cavities known as haloscopes. Traditionally, haloscopes consist of tunable copper cavities operating in the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:msub><a:mrow><a:mi>TM</a:mi></a:mrow><a:mrow><a:mn>010</a:mn></a:mrow></a:msub></a:mrow></a:math> mode, but ohmic losses have limited their performance. In contrast, superconducting radio frequency (SRF) cavities can achieve quality factors of <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mrow><c:mo>∼</c:mo><c:msup><c:mrow><c:mn>10</c:mn></c:mrow><c:mrow><c:mn>10</c:mn></c:mrow></c:msup></c:mrow></c:math>, perhaps 5 orders of magnitude better than copper cavities, leading to more sensitive dark matter detectors. In this paper, we first derive that the scan rate of a haloscope experiment is proportional to the loaded quality factor <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mrow><e:msub><e:mrow><e:mi>Q</e:mi></e:mrow><e:mrow><e:mi mathvariant="normal">L</e:mi></e:mrow></e:msub></e:mrow></e:math>, even if the cavity bandwidth is much narrower than the dark matter halo line shape. We then present a proof-of-concept search for dark photon dark matter using a nontunable ultrahigh-quality SRF cavity. We exclude dark photon dark matter with kinetic mixing strengths of <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mrow><h:mi>χ</h:mi><h:mo>&gt;</h:mo><h:mn>1.5</h:mn><h:mo>×</h:mo><h:msup><h:mrow><h:mn>10</h:mn></h:mrow><h:mrow><h:mo>−</h:mo><h:mn>16</h:mn></h:mrow></h:msup></h:mrow></h:math> for a dark photon mass of <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:mrow><j:msub><j:mrow><j:mi>m</j:mi></j:mrow><j:mrow><j:msup><j:mrow><j:mi>A</j:mi></j:mrow><j:mrow><j:mo>′</j:mo></j:mrow></j:msup></j:mrow></j:msub><j:mo>=</j:mo><j:mn>5.35</j:mn><j:mtext> </j:mtext><j:mtext> </j:mtext><j:mrow><j:mi mathvariant="normal">μ</j:mi><j:mi>eV</j:mi></j:mrow></j:mrow></j:math>, achieving the deepest exclusion to wavelike dark photons by almost an order of magnitude. Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(4)
Fermi National Accelerator Laboratory (US), National Institute of Standards and Technology (US), University of Padua (IT), Istituto Nazionale di Fisica Nucleare, Sezione di Padova (IT), National Institute of Standards (EG)
U.S. Department of Energy, Office of Science
Openalex Percentile: Top 2%
Dark Matter and Cosmic Phenomena
8.58
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