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Search for dark-matter axions beyond the quantum limit: The cosmological axion Sarov haloscope proposal

A. L. PankratovNizhny Novgorod State Pedagogical UniversityPavel A. BelovITMO UniversityE. BoosMoscow State UniversityA.S. ChepurnovLomonosov Moscow State UniversityA. V. ChiginevNizhny Novgorod State Technical University n. a. R. E. AlekseevA. DerbinPetersburg Nuclear Physics Institute NRC KII. DrachnevPetersburg Nuclear Physics Institute NRC KIL. DudkoMoscow State UniversityDmitry GorbunovInstitute for Nuclear Research of the Russian Academy of SciencesMaxim A. GorlachITMO UniversityVadim V. IvanovNizhny Novgorod State Pedagogical UniversityL. KravchukInstitute for Nuclear Research of the Russian Academy of SciencesMaxim LibanovMoscow Institute of Physics and TechnologyM. MerkinMoscow State UniversityV. MuratovaPetersburg Nuclear Physics Institute NRC KIAlexander PukhovMoscow State UniversityDmitry SalnikovMoscow State UniversityPetr SatuninInstitute for Nuclear Research of the Russian Academy of SciencesD. A. SemenovPetersburg Nuclear Physics Institute NRC KIA. SergeevGaponov-Grekhov Institute of Applied Physics of the Russian Academy of SciencesMaksim I. StarostinLomonosov Moscow State UniversityI. TkachevInstitute for Nuclear Research of the Russian Academy of SciencesS. TroitskyInstitute for Nuclear Research of the Russian Academy of SciencesМ. В. ТрушинPetersburg Nuclear Physics Institute NRC KIE. UnzhakovPetersburg Nuclear Physics Institute NRC KIMaxim VyalkovBranch of Lomonosov Moscow State University in SarovA. A. YukhimchukAll-Russian Scientific Research Institute of Technical Physics
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Firmly established in astrophysical observations, dark matter evades direct detection in experiments. Axions and axionlike particles are among the leading dark-matter candidates, and numerous attempts to detect them in laboratories have been performed. Here, we propose to advance these efforts substantially, extending the sensitivity for dark-matter axions in the mass range <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mo stretchy="false">(</a:mo><a:mn>38</a:mn><a:mi>–</a:mi><a:mn>54</a:mn><a:mo stretchy="false">)</a:mo><a:mtext> </a:mtext><a:mtext> </a:mtext><a:mi mathvariant="normal">μ</a:mi><a:mi>eV</a:mi></a:mrow></a:math> down to the axion-photon couplings <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"><f:msub><f:mi>g</f:mi><f:mrow><f:mi>a</f:mi><f:mi>γ</f:mi><f:mi>γ</f:mi></f:mrow></f:msub><f:mo>≲</f:mo><f:mrow><f:mo stretchy="false">(</f:mo><f:msup><f:mn>10</f:mn><f:mrow><f:mo>−</f:mo><f:mn>14</f:mn></f:mrow></f:msup><f:mo>−</f:mo><f:msup><f:mn>10</f:mn><f:mrow><f:mo>−</f:mo><f:mn>15</f:mn></f:mrow></f:msup><f:mo stretchy="false">)</f:mo></f:mrow><f:mtext> </f:mtext><f:mtext> </f:mtext><f:msup><f:mi>GeV</f:mi><f:mrow><f:mo>−</f:mo><f:mn>1</f:mn></f:mrow></f:msup></f:math>, motivated by generic models of quantum chromodynamics axion. Single-photon detectors operating at ultralow temperatures are key elements of the experiment. The projected sensitivity will be reached in one year of data taking with magnetic field of (1–10) T, making Cosmological Axion Sarov Haloscope (CASH) the most sensitive haloscope in this mass range.

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