Nuclear magnetic resonance dark-matter searches are sensitive to dark photons and the axion-photon coupling

We demonstrate that nuclear magnetic resonance based searches for dark matter (DM) have intrinsic and powerful sensitivity to dark photons and the axion-photon coupling. The reason is conceptually straightforward. An instrument such as CASPEr-Gradient begins with a large sample of nuclear spins polarized in a background magnetic field. In the presence of axion DM coupled to nucleons, the spin ensemble feels an effective magnetic field <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mi mathvariant="bold">B</a:mi> <a:mo>∝</a:mo> <a:mo>∇</a:mo> <a:mi>a</a:mi> </a:mrow> </a:math> that tilts the spins, generating a potentially observable precession. If the magnetic field is real rather than effective, the system responds identically. A real field can be generated by a kinetically mixed dark photon within the shielded region the sample is placed or an axion coupled to photons through its interaction with the background magnetic field. We show that all three signals are detectable and distinguishable. If CASPEr-Gradient were to reach the QCD axion prediction of the axion-nucleon coupling, it would simultaneously be sensitive to kinetic mixings of <d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline"> <d:mrow> <d:mi>ε</d:mi> <d:mo>≃</d:mo> <d:mn>3</d:mn> <d:mo>×</d:mo> <d:msup> <d:mrow> <d:mn>10</d:mn> </d:mrow> <d:mrow> <d:mo>−</d:mo> <d:mn>16</d:mn> </d:mrow> </d:msup> </d:mrow> </d:math> and axion-photon couplings of <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"> <f:mrow> <f:msub> <f:mrow> <f:mi>g</f:mi> </f:mrow> <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:mn>2</f:mn> <f:mo>×</f:mo> <f:msup> <f:mrow> <f:mn>10</f:mn> </f:mrow> <f:mrow> <f:mo>−</f:mo> <f:mn>16</f:mn> </f:mrow> </f:msup> <f:mtext> </f:mtext> <f:mtext> </f:mtext> <f:msup> <f:mrow> <f:mi>GeV</f:mi> </f:mrow> <f:mrow> <f:mo>−</f:mo> <f:mn>1</f:mn> </f:mrow> </f:msup> </f:mrow> </f:math> for <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"> <h:mi>m</h:mi> <h:mo>≃</h:mo> <h:mn>1</h:mn> <h:mtext> </h:mtext> <h:mtext> </h:mtext> <h:mi>μ</h:mi> <h:mi>eV</h:mi> </h:math> . Our analysis demonstrates that CASPEr-Gradient has the tantalizing possibility of measuring two separate couplings of axion dark matter, thereby providing a unique window into the axion’s UV completion.

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Journal
Physical review. D/Physical review. D.
Published
2026-01-21
DOI
https://doi.org/10.1103/f9fj-6kkj
Primary Topic
Dark Matter and Cosmic Phenomena
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article
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article

Nuclear magnetic resonance dark-matter searches are sensitive to dark photons and the axion-photon coupling

Jacob M. Leedom, Sebastian A. R. Ellis, Anonymous, Nicholas L. Rodd
Physical review. D/Physical review. D.
Dark Matter and Cosmic Phenomena
article

Nuclear magnetic resonance dark-matter searches are sensitive to dark photons and the axion-photon coupling

Jacob M. Leedom, Sebastian A. R. Ellis, Anonymous, Nicholas L. Rodd
article en

Abstract

We demonstrate that nuclear magnetic resonance based searches for dark matter (DM) have intrinsic and powerful sensitivity to dark photons and the axion-photon coupling. The reason is conceptually straightforward. An instrument such as CASPEr-Gradient begins with a large sample of nuclear spins polarized in a background magnetic field. In the presence of axion DM coupled to nucleons, the spin ensemble feels an effective magnetic field <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mi mathvariant="bold">B</a:mi> <a:mo>∝</a:mo> <a:mo>∇</a:mo> <a:mi>a</a:mi> </a:mrow> </a:math> that tilts the spins, generating a potentially observable precession. If the magnetic field is real rather than effective, the system responds identically. A real field can be generated by a kinetically mixed dark photon within the shielded region the sample is placed or an axion coupled to photons through its interaction with the background magnetic field. We show that all three signals are detectable and distinguishable. If CASPEr-Gradient were to reach the QCD axion prediction of the axion-nucleon coupling, it would simultaneously be sensitive to kinetic mixings of <d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline"> <d:mrow> <d:mi>ε</d:mi> <d:mo>≃</d:mo> <d:mn>3</d:mn> <d:mo>×</d:mo> <d:msup> <d:mrow> <d:mn>10</d:mn> </d:mrow> <d:mrow> <d:mo>−</d:mo> <d:mn>16</d:mn> </d:mrow> </d:msup> </d:mrow> </d:math> and axion-photon couplings of <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"> <f:mrow> <f:msub> <f:mrow> <f:mi>g</f:mi> </f:mrow> <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:mn>2</f:mn> <f:mo>×</f:mo> <f:msup> <f:mrow> <f:mn>10</f:mn> </f:mrow> <f:mrow> <f:mo>−</f:mo> <f:mn>16</f:mn> </f:mrow> </f:msup> <f:mtext> </f:mtext> <f:mtext> </f:mtext> <f:msup> <f:mrow> <f:mi>GeV</f:mi> </f:mrow> <f:mrow> <f:mo>−</f:mo> <f:mn>1</f:mn> </f:mrow> </f:msup> </f:mrow> </f:math> for <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"> <h:mi>m</h:mi> <h:mo>≃</h:mo> <h:mn>1</h:mn> <h:mtext> </h:mtext> <h:mtext> </h:mtext> <h:mi>μ</h:mi> <h:mi>eV</h:mi> </h:math> . Our analysis demonstrates that CASPEr-Gradient has the tantalizing possibility of measuring two separate couplings of axion dark matter, thereby providing a unique window into the axion’s UV completion.

Physical review. D/Physical review. D.Vol. 113(3)
University of Geneva (CH), Lawrence Berkeley National Laboratory (US), FZU ‒ Institute of Physics of the Academy of Sciences of the Czech Republic (CZ), University of California, Berkeley (US)
Openalex Percentile: Top 76%
Dark Matter and Cosmic Phenomena
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