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

A. L. PankratovInstitute for Physics of Microstructures of RASPavel A. BelovITMO UniversityE. BoosLomonosov Moscow State UniversityA.S. ChepurnovLomonosov Moscow State UniversityA. V. ChiginevInstitute for Physics of Microstructures of RASA. DerbinNational Research Centre Kurchatov InstituteI. DrachnevPetersburg Nuclear Physics Institute NRC KIL. DudkoLomonosov Moscow State UniversityDmitry GorbunovInstitute for Nuclear Research of the Russian Academy of SciencesMaxim A. GorlachITMO UniversityVadim V. IvanovInstitute for Physics of Microstructures of RASL. KravchukInstitute for Nuclear Research of the Russian Academy of SciencesMaxim LibanovInstitute for Nuclear Research of the Russian Academy of SciencesM. MerkinLomonosov Moscow State UniversityV. MuratovaPetersburg Nuclear Physics Institute NRC KIAlexander PukhovLomonosov Moscow State UniversityDmitry SalnikovInstitute for Nuclear Research of the Russian Academy of SciencesPetr 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. StarostinBranch of Lomonosov Moscow State University in SarovI. 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. YukhimchukRussian Federal Nuclear Center-All-Russian Scientific Research Institute of Experimental Physics
ABI

Аннотация

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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