184(m,g)Re cross sections and isomeric ratios in181Ta(α, n) and W(α, pxn) reactions

1993 ◽  
Vol 172 (1) ◽  
pp. 155-165 ◽  
Author(s):  
M. J. Ozafran ◽  
H. O. Mosca ◽  
M. E. Vazquez ◽  
W. R. Frosch ◽  
S. J. Nassiff
1976 ◽  
Vol 23 (3-4) ◽  
Author(s):  
O. HERREROS USHER ◽  
C. M. ARIZMENDI ◽  
C. WASILEVSKY ◽  
S. J. NASSIFF

1989 ◽  
Vol 137 (3) ◽  
pp. 173-182 ◽  
Author(s):  
M. J. Ozafran ◽  
H. O. Mosca ◽  
M. E. Vazquez ◽  
S. J. Nassiff

2002 ◽  
Vol 65 (5) ◽  
pp. 776-784 ◽  
Author(s):  
V. É. Aleksandryan ◽  
J. Adam ◽  
A. R. Balabekyan ◽  
A. S. Danagulyan ◽  
V. G. Kalinnikov ◽  
...  

2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Junhua Luo ◽  
Li Jiang

Abstract The (n,α) and (n,p) cross-sections and their isomeric ratios (σ m /σ g ) were measured at 13–15 MeV for 92Mo and 95Mo by activation and off-line γ-ray spectrometry. The activated Mo samples combined with Al foils were used to obtain the cross-section values and the neutron flux, generated using the 3H(d,n)4He reaction. The cross-sections of the ground states were obtained using the metastable state absolute cross-sections and the residual nuclear decay rule. The excitation functions, total cross-sections, and isomeric ratios for the 92Mo(n,α)89m,gZr and 95Mo(n,p)95m,gNb reactions were calculated using the TALYS-1.95 software. 92Mo(n,α)89m + gZr and 95Mo(n,p)95m + gNb reaction excitation functions were obtained using the EMPIRE-3.2.3 package. These simulation results were compared with the corresponding experimental data and with the evaluated data from the ENDF/B-VIII.0, JEFF-3.3, CENDL-3, and ROSFOND libraries. Only partial agreements were observed.


1996 ◽  
Vol 207 (1) ◽  
pp. 45-52 ◽  
Author(s):  
F. P. De La Cruz ◽  
A. J. Moreno ◽  
S. J. Nassiff

1993 ◽  
Vol 345 (3) ◽  
pp. 285-292 ◽  
Author(s):  
A. Kirov ◽  
N. Nenoff ◽  
E. Georgieva ◽  
C. Necheva ◽  
I. Ephtimov

1987 ◽  
Vol 62 (4) ◽  
pp. 277-285 ◽  
Author(s):  
M. G. Davydov ◽  
V. G. Magera ◽  
A. V. Trukhov

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