2009
DOI: 10.1140/epjc/s10052-009-1095-y
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Search for resonant absorption of solar axions emitted in M1 transition in 57Fe nuclei

Abstract: A search for resonant absorption of 14.4 keV solar axions by a 57 Fe target was performed. The Si(Li) detector placed inside the low-background setup was used to detect the γ -quanta appearing in the deexcitation of the 14.4 keV nuclear level: A + 57 Fe → 57 Fe * → 57 Fe + γ . The new upper limit for the hadronic axion mass has been obtained of m A ≤ 159 eV (95% c.l.) (S = 0.5, z = 0.56).

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Cited by 27 publications
(19 citation statements)
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“…More relevant in the present context are the constraints obtained from supernova SN1987A [35] or the metallicity of red giant stars [36], which limit axion-nucleon interactions. The 14.4 keV emission line of 57 Fe also constrains axionnucleon couplings [37]. However, these astrophysical constraints are somewhat particular to the axion, and do not apply to other pseudoscalar bosons or axial-vector interactions [9,38].…”
mentioning
confidence: 99%
“…More relevant in the present context are the constraints obtained from supernova SN1987A [35] or the metallicity of red giant stars [36], which limit axion-nucleon interactions. The 14.4 keV emission line of 57 Fe also constrains axionnucleon couplings [37]. However, these astrophysical constraints are somewhat particular to the axion, and do not apply to other pseudoscalar bosons or axial-vector interactions [9,38].…”
mentioning
confidence: 99%
“…[24][25][26][27][28][29][30][31][32][33][34][35][36][37][38][39]. The strongest limit for the hadronic axion mass (m A 151 eV) was made for 14.4 keV axions emitted in the M1 transition of a 57 Fe nucleus [36]. A significant advantage of our experiment is that for the M1 transition of 169 Tm the !…”
Section: Resultsmentioning
confidence: 99%
“…As discussed in Sec. I, within the model of hadronic axions, whose coupling constant is a function of m a , the upper limits for the axion mass m a ≤ 159 eV [20] and m a ≤ 145 eV [21] were obtained using the detector of γ-quanta appearing in the deexcitation of the nuclear level excited by solar axions. The parameters of hadronic axions were also found from the neutrino data of supernova SN 1987A [22] and from astrophysical arguments connected with stellar cooling by the axion emission [23,24].…”
Section: Straintsmentioning
confidence: 99%
“…These interactions are used for experimental searches of axion-like particles in both the laboratory experiments (see below) and in astrophysics (see, for instance, constraints on the axion-photon and axionelectron coupling constants obtained by means of axion solar telescope [17] and from the Compton process and electron-positron annihilation with an axion emission in stellar plasmas [18,19], respectively). Both the laboratory and astrophysical constraints may depend on the model of axions used containing different relations between couplings to different particles (for instance, the constraints from the solar axion data [20,21] and from the neutrino data of supernova SN 1987A [22] are found using the model of hadronic axions, where the coupling constant is a function of the axion mass). The astrophysical constraints may also depend on complicated behavior of matter in stars.…”
Section: Introductionmentioning
confidence: 99%
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