Probing the axion-nucleon coupling with supergiant stars

A finite axion-nucleon coupling enables the production of axions in stellar environments via the thermal excitation and subsequent deexcitation of the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mmultiscripts> <a:mrow> <a:mi>Fe</a:mi> </a:mrow> <a:mprescripts/> <a:none/> <a:mrow> <a:mn>57</a:mn> </a:mrow> </a:mmultiscripts> </a:mrow> </a:math> isotope. Given its low-lying excited state at 14.4 keV, <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:mmultiscripts> <c:mrow> <c:mi>Fe</c:mi> </c:mrow> <c:mprescripts/> <c:none/> <c:mrow> <c:mn>57</c:mn> </c:mrow> </c:mmultiscripts> </c:mrow> </c:math> can be efficiently excited in the hot cores of supergiant stars, possibly leading to axion emission. The conversion of these axions into photons in the Galactic magnetic field results in a characteristic 14.4 keV line, potentially detectable by hard x-ray telescopes such as NASA’s Nuclear Spectroscopic Telescope Array (u). In this work, we present the first constraints on axion-nucleon couplings derived from u observations of Betelgeuse and discuss the potential insights that could be gained from detecting this line in other nearby supergiants. Our results establish significantly more stringent bounds than those obtained from solar observations, setting a limit of <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mo stretchy="false">|</e:mo> <e:msub> <e:mi>g</e:mi> <e:mrow> <e:mi>a</e:mi> <e:mi>γ</e:mi> </e:mrow> </e:msub> <e:msubsup> <e:mi>g</e:mi> <e:mrow> <e:mi>a</e:mi> <e:mi>N</e:mi> </e:mrow> <e:mi>eff</e:mi> </e:msubsup> <e:mo stretchy="false">|</e:mo> <e:mo>&lt;</e:mo> <e:mo stretchy="false">(</e:mo> <e:mn>1.2</e:mn> <e:mi>–</e:mi> <e:mn>2.7</e:mn> <e:mo stretchy="false">)</e:mo> <e:mo>×</e:mo> <e:msup> <e:mn>10</e:mn> <e:mrow> <e:mo>−</e:mo> <e:mn>20</e:mn> </e:mrow> </e:msup> <e:mtext> </e:mtext> <e:mtext> </e:mtext> <e:mrow> <e:msup> <e:mrow> <e:mi>GeV</e:mi> </e:mrow> <e:mrow> <e:mo>−</e:mo> <e:mn>1</e:mn> </e:mrow> </e:msup> </e:mrow> </e:math> for <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:msub> <k:mi>m</k:mi> <k:mi>a</k:mi> </k:msub> <k:mo>≲</k:mo> <k:msup> <k:mn>10</k:mn> <k:mrow> <k:mo>−</k:mo> <k:mn>10</k:mn> </k:mrow> </k:msup> <k:mtext> </k:mtext> <k:mtext> </k:mtext> <k:mi>eV</k:mi> </k:math> .

Authors

Institutions

Publication Details

Journal
Physical review. D/Physical review. D.
Published
2025-12-05
DOI
https://doi.org/10.1103/xv5c-j2rv
Citations
1
Primary Topic
Dark Matter and Cosmic Phenomena
Type
article
Field-Weighted Citation Impact
1.87
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

Probing the axion-nucleon coupling with supergiant stars

Karl J. Friston
1 citations
Physical review. D/Physical review. D.
Dark Matter and Cosmic Phenomena
1.87
article

Probing the axion-nucleon coupling with supergiant stars

Karl J. Friston
article en
1 citations

Abstract

A finite axion-nucleon coupling enables the production of axions in stellar environments via the thermal excitation and subsequent deexcitation of the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mmultiscripts> <a:mrow> <a:mi>Fe</a:mi> </a:mrow> <a:mprescripts/> <a:none/> <a:mrow> <a:mn>57</a:mn> </a:mrow> </a:mmultiscripts> </a:mrow> </a:math> isotope. Given its low-lying excited state at 14.4 keV, <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:mmultiscripts> <c:mrow> <c:mi>Fe</c:mi> </c:mrow> <c:mprescripts/> <c:none/> <c:mrow> <c:mn>57</c:mn> </c:mrow> </c:mmultiscripts> </c:mrow> </c:math> can be efficiently excited in the hot cores of supergiant stars, possibly leading to axion emission. The conversion of these axions into photons in the Galactic magnetic field results in a characteristic 14.4 keV line, potentially detectable by hard x-ray telescopes such as NASA’s Nuclear Spectroscopic Telescope Array (u). In this work, we present the first constraints on axion-nucleon couplings derived from u observations of Betelgeuse and discuss the potential insights that could be gained from detecting this line in other nearby supergiants. Our results establish significantly more stringent bounds than those obtained from solar observations, setting a limit of <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mo stretchy="false">|</e:mo> <e:msub> <e:mi>g</e:mi> <e:mrow> <e:mi>a</e:mi> <e:mi>γ</e:mi> </e:mrow> </e:msub> <e:msubsup> <e:mi>g</e:mi> <e:mrow> <e:mi>a</e:mi> <e:mi>N</e:mi> </e:mrow> <e:mi>eff</e:mi> </e:msubsup> <e:mo stretchy="false">|</e:mo> <e:mo>&lt;</e:mo> <e:mo stretchy="false">(</e:mo> <e:mn>1.2</e:mn> <e:mi>–</e:mi> <e:mn>2.7</e:mn> <e:mo stretchy="false">)</e:mo> <e:mo>×</e:mo> <e:msup> <e:mn>10</e:mn> <e:mrow> <e:mo>−</e:mo> <e:mn>20</e:mn> </e:mrow> </e:msup> <e:mtext> </e:mtext> <e:mtext> </e:mtext> <e:mrow> <e:msup> <e:mrow> <e:mi>GeV</e:mi> </e:mrow> <e:mrow> <e:mo>−</e:mo> <e:mn>1</e:mn> </e:mrow> </e:msup> </e:mrow> </e:math> for <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:msub> <k:mi>m</k:mi> <k:mi>a</k:mi> </k:msub> <k:mo>≲</k:mo> <k:msup> <k:mn>10</k:mn> <k:mrow> <k:mo>−</k:mo> <k:mn>10</k:mn> </k:mrow> </k:msup> <k:mtext> </k:mtext> <k:mtext> </k:mtext> <k:mi>eV</k:mi> </k:math> .

Physical review. D/Physical review. D.Vol. 112(12)
TU Dortmund University (DE), Universidad de Zaragoza (ES), Canadian Arthritis Patient Alliance (CA)
Openalex Percentile: Top 10%
Dark Matter and Cosmic Phenomena
1.87
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.