scholarly journals Two-phase emission detector for measuring coherent neutrino-nucleus scattering

2004 ◽  
Vol 51 (5) ◽  
pp. 2151-2155 ◽  
Author(s):  
C. Hagmann ◽  
A. Bernstein
2013 ◽  
Vol 8 (05) ◽  
pp. P05017-P05017 ◽  
Author(s):  
D Yu Akimov ◽  
A V Akindinov ◽  
I S Alexandrov ◽  
V A Belov ◽  
A I Bolozdynya ◽  
...  

2020 ◽  
Vol 15 (02) ◽  
pp. P02020-P02020 ◽  
Author(s):  
D.Y. Akimov ◽  
V.A. Belov ◽  
A.I. Bolozdynya ◽  
A.G. Dolgolenko ◽  
Y.V. Efremenko ◽  
...  

2013 ◽  
Vol 8 (10) ◽  
pp. P10023-P10023 ◽  
Author(s):  
D Yu Akimov ◽  
I S Alexandrov ◽  
V I Aleshin ◽  
V A Belov ◽  
A I Bolozdynya ◽  
...  

2016 ◽  
Vol 11 (12) ◽  
pp. P12005-P12005 ◽  
Author(s):  
D.Yu. Akimov ◽  
V.A. Belov ◽  
A.I. Bolozdynya ◽  
V.A. Kaplin ◽  
A.V. Khromov ◽  
...  
Keyword(s):  

2018 ◽  
Vol 174 ◽  
pp. 02005
Author(s):  
A. Bondar ◽  
A. Buzulutskov ◽  
A. Dolgov ◽  
E. Shemyakina ◽  
A. Sokolov

Two-phase Cryogenic Avalanche Detectors (CRADs) with combined THGEM/GAPD-matrix multiplier have become an emerging technique in rare-event experiments such as those of coherent neutrino-nucleus scattering and dark matter search. In this work we continue to study the performance of the two-phase CRAD in Ar with THGEM/GAPD-matrix charge/optical readout. The matrix was composed of a 3×3 array of GAPDs (Geiger-mode APDs), optically recording THGEM-hole avalanches in the Near Infrared (NIR). Gain, time, amplitude and spatial resolution properties of the combined multiplier are described.


2019 ◽  
Vol 62 (4) ◽  
pp. 457-463 ◽  
Author(s):  
D. Yu. Akimov ◽  
V. A. Belov ◽  
A. I. Bolozdynya ◽  
A. A. Vasin ◽  
A. V. Galavanov ◽  
...  

2017 ◽  
Vol 60 (2) ◽  
pp. 175-181 ◽  
Author(s):  
D. Yu. Akimov ◽  
I. S. Aleksandrov ◽  
V. A. Belov ◽  
A. I. Bolozdynya ◽  
A. A. Burenkov ◽  
...  
Keyword(s):  

Author(s):  
K. P. Staudhammer ◽  
L. E. Murr

The effect of shock loading on a variety of steels has been reviewed recently by Leslie. It is generally observed that significant changes in microstructure and microhardness are produced by explosive shock deformation. While the effect of shock loading on austenitic, ferritic, martensitic, and pearlitic structures has been investigated, there have been no systematic studies of the shock-loading of microduplex structures.In the current investigation, the shock-loading response of millrolled and heat-treated Uniloy 326 (thickness 60 mil) having a residual grain size of 1 to 2μ before shock loading was studied. Uniloy 326 is a two phase (microduplex) alloy consisting of 30% austenite (γ) in a ferrite (α) matrix; with the composition.3% Ti, 1% Mn, .6% Si,.05% C, 6% Ni, 26% Cr, balance Fe.


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