14 research outputs found

    Search for axioelectric effect of 5.5 MeV solar axions using BGO detectors

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    A search for axioelectric absorption of solar axions produced in the p+d→3He+γ(5.5MeV) p + d \rightarrow {^3\rm{He}}+\gamma (5.5 \rm{MeV}) reactions has been performed with a BGO detector placed in a low-background setup. A model-independent limit on an axion-nucleon and axion-electron coupling constant has been obtained: ∣gAe×gAN3∣<2.9×10−9| g_{Ae}\times g_{AN}^3|< 2.9\times 10^{-9} for 90% confidence level. The constrains of the axion-electron coupling have been obtained for hadronic axion with masses in (0.1 - 1) MeV range: ∣gAe∣≤(1.4−9.7)×10−7|g_{Ae}| \leq (1.4 - 9.7)\times 10^{-7}.Comment: 6 pages, 4 figures, to be published in EPJ C. arXiv admin note: substantial text overlap with arXiv:1007.338

    Searches for axioelectric effect of solar axions with BGO-scintillator and BGO-bolometer detectors

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    A search for axioelectric absorption of 5.5 MeV solar axions produced in the p+d→3He+γ (5.5 MeV)p + d \rightarrow {^3\rm{He}}+\gamma~(5.5~ \rm{MeV}) reaction has been performed with a BGO detectors. A model-independent limit on the product of axion-nucleon gAN3g_{AN}^3 and axion-electron gAeg_{Ae} coupling constants has been obtained: ∣gAe×gAN3∣<1.9×10−10| g_{Ae}\times g_{AN}^3|< 1.9\times 10^{-10} for 90\% C.L..Comment: 5 pages, 3 figures, Proceedings of the 10th Patras Workshop on Axions, WIMPs and WISP 29 June - 4 July 2014, CERN, Geneva, Switzerlan

    New limits on the resonant absorption of solar axions obtained with a 169^{169}Tm-containing cryogenic detector

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    A search for resonant absorption of solar axions by 169^{169}Tm nuclei was carried out. A newly developed approach involving low-background cryogenic bolometer based on Tm3_3Al5_5O12_{12} crystal was used that allowed for significant improvement of sensitivity in comparison with previous 169^{169}Tm based experiments. The measurements performed with 8.188.18 g crystal during 6.66.6 days exposure yielded the following limits on axion couplings: ∣gAγ(gAN0+gAN3)≤1.44×10−14|g_{A\gamma} (g_{AN}^0 + g_{AN}^3) \leq 1.44 \times 10^{-14} GeV−1^{-1} and ∣gAe(gAN0+gAN3)≤2.81×10−16|g_{Ae} (g_{AN}^0 + g_{AN}^3) \leq 2.81 \times 10^{-16}.Comment: 7 pages, 5 figure

    Measurement of 144Pr^{144}\rm{Pr} beta-spectrum with Si(Li) detectors for the purpose of determining the spectrum of electron antineutrinos

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    Here we present the specifications of the newly developed beta-spectrometer based on thick full absorption Si(Li) detector. The spectrometer can be used for precision measurements of various beta-spectra, namely for the beta-spectrum shape study of 144^{144}Pr, which is considered to be the most promising anti-neutrino source for sterile neutrino searches
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