The determination of the 93Nb (n, n′)93mNb excitation function using foil activation

1986 ◽  
Vol 93 (1-4) ◽  
pp. 185-188 ◽  
Author(s):  
Derek B. Gayther ◽  
Michael F. Murphy ◽  
Keith Randle ◽  
William H. Taylor ◽  
Connell A. Uttley
2021 ◽  
Vol 104 (1) ◽  
Author(s):  
M. Veicht ◽  
I. Kajan ◽  
J.-C. David ◽  
S. Chen ◽  
E. Strub ◽  
...  
Keyword(s):  

2018 ◽  
Vol 318 (1) ◽  
pp. 375-380
Author(s):  
John J. Goodell ◽  
Christine M. Egnatuk ◽  
Stephen W. Padgett ◽  
Bryan B. Bandong ◽  
Kevin E. Roberts ◽  
...  

1993 ◽  
Vol 71 (3-4) ◽  
pp. 115-121 ◽  
Author(s):  
N. L. Singh ◽  
S. Agarwal ◽  
J. Rama Rao

The excitation functions of 51V [(α, xn), x = 1.3; (α, p3n); (α, α3n) (α, 2α)] and 59Co[(α, 2n); (α, αxn); x = 1, 2] reactions were measured up to 50 MeV by the stacked-foil activation technique and high-resolution Ce(Li)–HPGe spectroscopy method. Of these 51V(α, xnypzα) reactions were studied for the first time with better accuracy than earlier measurements, which were done with a poor resolution scintillation–Ge(Li) detectors some 20 years ago. In the case of 59Co, existing data show large discrepancies at low energy. Comparisons are presented with the prediction of hybrid and exciton models. While for the (α, xn) type of reactions, reasonably explainable pre-equilibrium contributions are found, there seem to be indications of direct inelastic scattering effects in the (α, αxn) type of reactions.


1994 ◽  
Vol 03 (01) ◽  
pp. 239-248 ◽  
Author(s):  
M.K. BHARDWAJ ◽  
I.A. RIZVI ◽  
A.K. CHAUBEY

The excitation function of α-induced reactions on 121Sb and 123Sb has been measured. The α-beam energy ranges from 55.0±0.5 MeV to 21.9±1.2 MeV. In these experiments, the stacked foil activation technique was used. The reaction yield was measured by counting the gamma ray activity produced by the alpha-induced reactions. Results so obtained were compared with the calculations from the geometry-dependent hybrid (GDH) model. The assumption of initial exciton number n0=4 with n=2, p=2 and h=0 best satisfies the results measured in the present work. The model calculations were done using the ALICE/LIVERMORE-82 computer code. The pre-equilibrium fraction has also been calculated.


1990 ◽  
Vol 247 (2-3) ◽  
pp. 242-245 ◽  
Author(s):  
J.B. Natowitz ◽  
M. Gonin ◽  
M. Gui ◽  
K. Hagel ◽  
Y. Lou ◽  
...  

Atomic Energy ◽  
1957 ◽  
Vol 2 (4) ◽  
pp. 474-476 ◽  
Author(s):  
V. A. Davidenko ◽  
I. S. Pogrebov ◽  
A. I. Saukov
Keyword(s):  

Author(s):  
Tayeb Kakavand ◽  
Morteza Taghilo ◽  
Mahdi Sadeghi

The 89Zr radioisotope is used in the field of tumor diagnostics, tumor therapy and the investigation of the biokinetic. The present work is investigated a suitable reaction to produce 89Zr..The Zirconium-89 excitation function via 89Y(p,n)89Zr, 89Y(d,2n)89Zr, natZr(p,pxn)89Zr, natSr(α,xn)89Zr and 90Zr(n,2n)89Zr reactions were calculated by ALICE-91 and TALYS-1.0 codes and the reaction of 89Y(p,n)89Zr has been selected. The calculated excitation function of 89Y(p,n)89Zr reaction was compared with the reported measurement and evaluations. Requisite thickness of targets was obtained by SRIM code for all above reactions except the 90Zr(n,2n)89Zr reaction. The 89Zr production yield was evaluated with attention to excitation function and stopping power for all above reactions except 90Zr(n,2n)89Zr reaction.


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