Determination of the half-life of the ground state ofTh229by usingU232andU233decay series

2011 ◽  
Vol 84 (1) ◽  
Author(s):  
H. Kikunaga ◽  
T. Suzuki ◽  
M. Nomura ◽  
T. Mitsugashira ◽  
A. Shinohara
Keyword(s):  
2016 ◽  
Vol 108 ◽  
pp. 143-147
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S.M. Collins ◽  
A.V. Harms ◽  
P.H. Regan
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1995 ◽  
Vol 200 (3) ◽  
pp. 223-225 ◽  
Author(s):  
M. S. Antony ◽  
D. Oster ◽  
M. S. Rouaban ◽  
A. Hachem

Author(s):  
E. Armengaud ◽  
C. Augier ◽  
A.  S. Barabash ◽  
F. Bellini ◽  
G. Benato ◽  
...  

Abstract We report the measurement of the two-neutrino double-beta ($$2\nu \beta \beta $$2νββ) decay of $$^{100}$$100Mo to the ground state of $$^{100}$$100Ru using lithium molybdate ($$\hbox {Li}_2^{\;\;100}\hbox {MoO}_4$$Li2100MoO4) scintillating bolometers. The detectors were developed for the CUPID-Mo program and operated at the EDELWEISS-III low background facility in the Modane underground laboratory (France). From a total exposure of 42.235 kg$$\times $$×day, the half-life of $$^{100}$$100Mo is determined to be $$T_{1/2}^{2\nu }=[7.12^{+0.18}_{-0.14}\,\mathrm {(stat.)}\pm 0.10\,\mathrm {(syst.)}]\times 10^{18}$$T1/22ν=[7.12-0.14+0.18(stat.)±0.10(syst.)]×1018 years. This is the most accurate determination of the $$2\nu \beta \beta $$2νββ half-life of $$^{100}$$100Mo to date.


1968 ◽  
Vol 58 (1) ◽  
pp. 232-246 ◽  
Author(s):  
F. Bella ◽  
M. Alessio ◽  
P. Fratelli
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1999 ◽  
Vol 6 (2) ◽  
pp. 211-220 ◽  
Author(s):  
A. Crubellier ◽  
O. Dulieu ◽  
F. Masnou-Seeuws ◽  
M. Elbs ◽  
H. Knöckel ◽  
...  

2002 ◽  
Vol 56 (1-2) ◽  
pp. 153-156 ◽  
Author(s):  
A. Grau Malonda ◽  
A. Grau Carles
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1991 ◽  
Vol 148 (2) ◽  
pp. 462-478 ◽  
Author(s):  
Thomas Nelis ◽  
Stuart P. Beaton ◽  
Kenneth M. Evenson ◽  
John M. Brown

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