We report the results of a search for axions from the 14.4 keV M1 transition from 57 Fe in the core of the sun using the axio-electric effect in TeO 2 bolometers. The detectors are 5 × 5 × 5 cm 3 crystals operated at about 10 mK in a facility used to test bolometers for the CUORE experiment at the Laboratori Nazionali del Gran Sasso in Italy. An analysis of 43.65 kg⋅d of data was made using a newly developed low energy trigger which was optimized to reduce the energy threshold of the detector. An upper limit of 0.58 c⋅kg −1 ⋅d −1 is established at 95% C.L., which translates into lower bounds f A ≥ 3.12 × 10 5 GeV 95% C.L. (DFSZ model) and f A ≥ 2.41 × 10 4 GeV 95% C.L. (KSVZ model) on the Peccei-Quinn symmetry-breaking scale, for a value of S = 0.5 of the flavor-singlet axial vector matrix element. These bounds can be expressed in terms of axion masses as m A ≤ 19.2 eV and m A ≤ 250 eV at 95% C.L. in the DFSZ and KSVZ models respectively. Bounds are given also for the interval 0.35 ≤ S ≤ 0.55.
Alessandria, F., Ardito, R., Artusa, D., Avignone III, F., Azzolini, O., Balata, M., et al. (2013). Search for 14.4 keV solar axions from M1 transition of 57 Fe with CUORE crystals. JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS, 2013(5) [10.1088/1475-7516/2013/05/007].
Search for 14.4 keV solar axions from M1 transition of 57 Fe with CUORE crystals
BIASSONI, MATTEO;BROFFERIO, CHIARA;Canonica, L;CAPELLI, SILVIA;CLEMENZA, MASSIMILIANO;Cremonesi, O;FERRI, ELENA;FIORINI, ETTORE;GIRONI, LUCA;GOTTI, CLAUDIO;MAINO, MATTEO;NUCCIOTTI, ANGELO ENRICO LODOVICO;Pattavina, L;PAVAN, MAURA;Previtali, E;SISTI, MONICA;ZANOTTI, LUIGI ERNESTO;
2013
Abstract
We report the results of a search for axions from the 14.4 keV M1 transition from 57 Fe in the core of the sun using the axio-electric effect in TeO 2 bolometers. The detectors are 5 × 5 × 5 cm 3 crystals operated at about 10 mK in a facility used to test bolometers for the CUORE experiment at the Laboratori Nazionali del Gran Sasso in Italy. An analysis of 43.65 kg⋅d of data was made using a newly developed low energy trigger which was optimized to reduce the energy threshold of the detector. An upper limit of 0.58 c⋅kg −1 ⋅d −1 is established at 95% C.L., which translates into lower bounds f A ≥ 3.12 × 10 5 GeV 95% C.L. (DFSZ model) and f A ≥ 2.41 × 10 4 GeV 95% C.L. (KSVZ model) on the Peccei-Quinn symmetry-breaking scale, for a value of S = 0.5 of the flavor-singlet axial vector matrix element. These bounds can be expressed in terms of axion masses as m A ≤ 19.2 eV and m A ≤ 250 eV at 95% C.L. in the DFSZ and KSVZ models respectively. Bounds are given also for the interval 0.35 ≤ S ≤ 0.55.File | Dimensione | Formato | |
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