Search for resonant absorption of solar axions emitted in M1-transitions in 83Kr nuclei: Second stage of the experiment

2018 ◽  
Vol 49 (1) ◽  
pp. 94-96 ◽  
Author(s):  
Yu. M. Gavrilyuk ◽  
A. M. Gangapshev ◽  
A. V. Derbin ◽  
V. V. Kazalov ◽  
V. V. Kuzminov ◽  
...  
2009 ◽  
Vol 62 (4) ◽  
pp. 755-760 ◽  
Author(s):  
A. V. Derbin ◽  
A. I. Egorov ◽  
I. A. Mitropol’sky ◽  
V. N. Muratova ◽  
D. A. Semenov ◽  
...  

2020 ◽  
Vol 638 ◽  
pp. A32 ◽  
Author(s):  
Q. M. Zhang ◽  
J. Dai ◽  
Z. Xu ◽  
D. Li ◽  
L. Lu ◽  
...  

Aims. We report our multiwavelength observations of two homologous circular-ribbon flares in active region 11991 on 2014 March 5, focusing on the transverse oscillations of an extreme-ultraviolet (EUV) loop excited by the flares. Methods. The flares were observed in ultraviolet and EUV wavelengths by the Atmospheric Imaging Assembly on board the Solar Dynamics Observatory spacecraft. These flares were also observed in Hα line center by the 1 m New Vacuum Solar Telescope. Soft X-ray fluxes of the flares in 0.5–4 and 1–8 Å were recorded by the GOES spacecraft. Results. The transverse oscillations are of fast standing kink mode. The first-stage oscillation triggered by the C2.8 flare is decayless with lower amplitudes (310–510 km). The periods (115–118 s) in different wavelengths are nearly the same, indicating coherent oscillations. The magnetic field of the loop is estimated to be 65–78 G. The second-stage oscillation triggered by the M1.0 flare is decaying with larger amplitudes (1250–1280 km). The periods decrease from 117 s in 211 Å to 70 s in 171 Å, implying a decrease of loop length or an implosion after a gradual expansion. The damping time, which is 147–315 s, increases with the period, so that the values of τ/P are close to each other in different wavelengths. The thickness of the inhomogeneous layer is estimated to be ∼0″​​​.45 under the assumption of resonant absorption. Conclusions. This is the first observation of the excitation of two kink-mode loop oscillations by two sympathetic flares. The results are important to understand the excitation of kink oscillations of coronal loops and hence the energy balance in the solar corona. Our findings also validate the prevalence of significantly amplified amplitudes of oscillations by successive drivers.


2009 ◽  
Vol 678 (2) ◽  
pp. 181-185 ◽  
Author(s):  
A.V. Derbin ◽  
S.V. Bakhlanov ◽  
A.I. Egorov ◽  
I.A. Mitropol'sky ◽  
V.N. Muratova ◽  
...  

2017 ◽  
Vol 934 ◽  
pp. 012018
Author(s):  
A V Derbin ◽  
I S Drachnev ◽  
A M Gangapshev ◽  
Yu M Gavrilyuk ◽  
V V Kazalov ◽  
...  

2007 ◽  
Vol 71 (6) ◽  
pp. 832-840 ◽  
Author(s):  
A. V. Derbin ◽  
A. I. Egorov ◽  
I. A. Mitropol’skii ◽  
V. N. Muratova

2020 ◽  
Vol 80 (5) ◽  
Author(s):  
A. H. Abdelhameed ◽  
S. V. Bakhlanov ◽  
P. Bauer ◽  
A. Bento ◽  
E. Bertoldo ◽  
...  

JETP Letters ◽  
2007 ◽  
Vol 85 (1) ◽  
pp. 12-16 ◽  
Author(s):  
A. V. Derbin ◽  
A. I. Egorov ◽  
I. A. Mitropol’sky ◽  
V. N. Muratova ◽  
N. V. Bazlov ◽  
...  

2012 ◽  
Vol 711 (1) ◽  
pp. 41-45 ◽  
Author(s):  
P. Belli ◽  
R. Bernabei ◽  
F. Cappella ◽  
R. Cerulli ◽  
F.A. Danevich ◽  
...  

2021 ◽  
Vol 2103 (1) ◽  
pp. 012142
Author(s):  
A H Abdelhameed ◽  
S V Bakhlanov ◽  
P Bauer ◽  
A Bento ◽  
E Bertoldo ◽  
...  

Abstract A newly developed experimental technique based on 169Tm-containing cryogenic bolometer detector was employed in order to perform the search for solar axions. The inclusion of target material into the active detector volume allowed for significant increase in sensitivity to axion parameters. A short 6.6 days measurement campaign with 8.18 g detector crystal yielded the following limits on axion couplings: | g A γ ( g A N 0 + g A N 3 ) ≤ 1.44 × 10 − 14 GeV − 1 and | g A e ( g A N 0 + g A N 3 ) ≤ 2.81 × 10 − 16 . The achieved results demonstrate high scalability potential of presented experimental approach.


1994 ◽  
Vol 144 ◽  
pp. 503-505
Author(s):  
R. Erdélyi ◽  
M. Goossens ◽  
S. Poedts

AbstractThe stationary state of resonant absorption of linear, MHD waves in cylindrical magnetic flux tubes is studied in viscous, compressible MHD with a numerical code using finite element discretization. The full viscosity tensor with the five viscosity coefficients as given by Braginskii is included in the analysis. Our computations reproduce the absorption rates obtained by Lou in scalar viscous MHD and Goossens and Poedts in resistive MHD, which guarantee the numerical accuracy of the tensorial viscous MHD code.


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