Decay time of heavy excited nuclei

2004 ◽  
Vol 734 ◽  
pp. 225-228 ◽  
Author(s):  
V.A. Drozdov ◽  
D.O. Eremenko ◽  
O.V. Fotina ◽  
G. Giardina ◽  
F. Malaguti ◽  
...  
Keyword(s):  
Author(s):  
D. O. EREMENKO ◽  
O. V. FOTINA ◽  
S. YU. PLATONOV ◽  
O. A. YUMINOV ◽  
G. GIARDINA ◽  
...  
Keyword(s):  

2003 ◽  
Vol 66 (9) ◽  
pp. 1628-1630 ◽  
Author(s):  
V. A. Drozdov ◽  
D. O. Eremenko ◽  
O. V. Fotina ◽  
S. Yu. Platonov ◽  
O. A. Yuminov
Keyword(s):  

2004 ◽  
Vol 31 (1) ◽  
pp. 29-37 ◽  
Author(s):  
M Jandel ◽  
A S Botvina ◽  
S J Yennello ◽  
G A Souliotis ◽  
D V Shetty ◽  
...  
Keyword(s):  

Author(s):  
V.A. Drozdov ◽  
D.O. Eremenko ◽  
O.V. Fotina ◽  
G. Giardina ◽  
F. Malaguti ◽  
...  
Keyword(s):  

1988 ◽  
Vol 53 (6) ◽  
pp. 1149-1155
Author(s):  
Jorge A. Bolzan

A simple method for optimization of the minimum decay time, previous to the sampling time of the polarographic current, is described. The former should make compatible two requisites: it should be short enough for obtaining the maximum value of the faradaic current and long enough for the minimum or null value of the double layer decay current. The method is performed with the pulse polarograph only, without ancillary instruments, is fast and its accuracy is fairly comparable with earlier methods, which were more accurate but by far more involved to perform.


2021 ◽  
pp. 118021
Author(s):  
Matthieu Hamel ◽  
Benoît Sabot ◽  
Chavdar Dutsov ◽  
Guillaume H.V. Bertrand ◽  
Krasimir Mitev
Keyword(s):  

2021 ◽  
Vol 1857 (1) ◽  
pp. 012013
Author(s):  
S Imagawa ◽  
H Kajitani ◽  
T Obana ◽  
S Takada ◽  
S Hamaguchi ◽  
...  

1964 ◽  
Vol 42 (11) ◽  
pp. 2173-2179 ◽  
Author(s):  
H. W. Taylor ◽  
T. A. Eastwood

A low-intensity peak has been found at 1010 ± 30 keV in the gamma-ray spectrum of 2.4-minute 108Ag obtained with NaI scintillation spectrometers. Consideration of the source-to-crystal distance as well as the effects of absorbers and decay time shows that it is the full-energy peak of a 1010 ± 30 keV gamma ray emitted by 108Ag. Gamma–gamma coincidence studies indicate that this gamma transition occurs between a new level at 1433 ± 30 and the 433-keV level of 108Pd.


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