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Is the Turner Window Open? Seeking Closure with Resonant Absorption of Galactic Axions in NaI Dark Matter Detectors

W. C. Haxton, Xing Liu, Anupam Ray, Evan Rule

Abstract

Motivated by the DAMA/LIBRA annual modulation signal, the dark matter community has invested heavily in ultra-clean underground NaI detectors to search for light WIMPs. We point out a new target of opportunity for these detectors -- axions produced by the carbon-burning stars within our galaxy. These stars synthesize large quantities of $^{23}$Na, keeping it at temperatures $\sim 10^9$K for periods up to tens of thousands of years. Under these conditions, $^{23}$Na radiates 440 keV axions through repeated photo-excitation and axio-deexcitation of its first excited state. Upon reaching a NaI detector, the process is reversed: the axion is resonantly absorbed, producing a 440 keV deexcitation photon. NaI thus serves as both $γ$ source and $γ$ detector. We find that existing NaI detectors can probe axion-nucleon couplings $|g_{aNN}^\mathrm{eff~^{23}Na}| \approx g_{app} \sim 10^{-6}$--$10^{-2}$, including QCD axions with $m_a \gtrsim 10$ eV. While there are several astrophysical constraints on axions with these couplings, our re-examination of these bounds shows that substantial gaps remain, providing strong motivation for the proposed searches.

Is the Turner Window Open? Seeking Closure with Resonant Absorption of Galactic Axions in NaI Dark Matter Detectors

Abstract

Motivated by the DAMA/LIBRA annual modulation signal, the dark matter community has invested heavily in ultra-clean underground NaI detectors to search for light WIMPs. We point out a new target of opportunity for these detectors -- axions produced by the carbon-burning stars within our galaxy. These stars synthesize large quantities of Na, keeping it at temperatures K for periods up to tens of thousands of years. Under these conditions, Na radiates 440 keV axions through repeated photo-excitation and axio-deexcitation of its first excited state. Upon reaching a NaI detector, the process is reversed: the axion is resonantly absorbed, producing a 440 keV deexcitation photon. NaI thus serves as both source and detector. We find that existing NaI detectors can probe axion-nucleon couplings --, including QCD axions with eV. While there are several astrophysical constraints on axions with these couplings, our re-examination of these bounds shows that substantial gaps remain, providing strong motivation for the proposed searches.
Paper Structure (1 section, 17 equations, 2 figures)

This paper contains 1 section, 17 equations, 2 figures.

Table of Contents

  1. Acknowledgments

Figures (2)

  • Figure 1: The axion emission probability (left, calculated for an 11$M_\odot$ progenitor), $^{23}$Na axion flux (middle), and the axion counts in a NaI experiment (right) as functions of $|g_{aNN}^\mathrm{eff~^{23}Na}|$. The shaded region is the $3\sigma$ exclusion for a 500 kg-yr NaI exposure. The dashed lines (obscured by the solid line in the left panel) result if resonant reabsorption is the only opacity source.
  • Figure 2: Potential exclusions on axion-nucleon couplings assuming a 500 kg-y NaI experiment (tan shaded). Existing astrophysical limits come from SNO (green), SN1987A KII $\gamma$ (red) and SN1987 cooling (blue). The SN1987A KII $\gamma$ exclusion contours correspond to 5, 15, 25, and 35 counts above background.