Table of Contents
Fetching ...

Experimental Search for Solar Axions via Coherent Primakoff Conversion in a Germanium Spectrometer

F. T. Avignone, D. Abriola, R. L. Brodzinski, J. I. Collar, R. J. Creswick, D. E. DiGregorio, H. A. Farach, A. O. Gattone, C. K. Guerard, F. Hasenbalg, H. Huck, H. S. Miley, A. Morales, J. Morales, S. Nussinov, A. Ortiz de Solorzano, J. H. Reeves, J. A. Villar, K. Zioutas

Abstract

Results are reported of an experimental search for the unique, rapidly varying temporal pattern of solar axions coherently converting into photons via the Primakoff effect in a single crystal germanium detector. This conversion is predicted when axions are incident at a Bragg angle with a crystalline plane. The analysis of approximately 1.94 kg.yr of data from the 1 kg DEMOS detector in Sierra Grande, Argentina, yields a new laboratory bound on axion-photon coupling of $g_{aγγ} < 2.7\cdot 10^{-9}$ GeV$^{-1}$, independent of axion mass up to ~ 1 keV.

Experimental Search for Solar Axions via Coherent Primakoff Conversion in a Germanium Spectrometer

Abstract

Results are reported of an experimental search for the unique, rapidly varying temporal pattern of solar axions coherently converting into photons via the Primakoff effect in a single crystal germanium detector. This conversion is predicted when axions are incident at a Bragg angle with a crystalline plane. The analysis of approximately 1.94 kg.yr of data from the 1 kg DEMOS detector in Sierra Grande, Argentina, yields a new laboratory bound on axion-photon coupling of GeV, independent of axion mass up to ~ 1 keV.

Paper Structure

This paper contains 17 equations, 5 figures.

Figures (5)

  • Figure 1: Feynman diagram of the Primakoff conversion of axions into photons.
  • Figure 2: A typical axion--photon conversion rate, $R(t,E)$, for various energy bands. The experimental energy resolution FWHM = 1.0 keV at 10 keV was used.
  • Figure 3: Scatter plot showing the distribution on the celestial sphere of all events between 4 keV and 8 keV over the data collection period of 707 days.
  • Figure 4: Values of $\lambda$ calculated from the 707 days of data as a function of the azimuthal angle $\phi$. The error bars are $1 \sigma$.
  • Figure 5: Exclusion plots on the $g_{a \gamma \gamma}$ vs. axion--mass plane. The curve to the left are from Ref. [16]. The letters indicate the following helium gas pressures in the conversion region of a strong magnetic field: (a) vacuum, (b) 55 Torr, and (c) 100 Torr.