235U(n, f) Fragment mass-, kinetic energy- and angular distributions for incident neutron energies between thermal and 6 MeV

1987 ◽  
Vol 462 (1) ◽  
pp. 85-108 ◽  
Author(s):  
Ch. Straede ◽  
C. Budtz-Jørgensen ◽  
H.-H. Knitter
1984 ◽  
Vol 29 (5) ◽  
pp. 1595-1605 ◽  
Author(s):  
A. Gökmen ◽  
H. Breuer ◽  
A. C. Mignerey ◽  
B. G. Glagola ◽  
K. Kwiatkowski ◽  
...  

2008 ◽  
Vol 17 (10) ◽  
pp. 2359-2362 ◽  
Author(s):  
E. BONNET ◽  
J. P. WIELECZKO ◽  
J. GOMEZ DEL CAMPO ◽  
M. LA COMMARA ◽  
S. BARLINI ◽  
...  

Cross sections, kinetic energy and angular distributions of fragments with charge 6 ≤ Z ≤ 28 emitted in 78,82 Kr +40 C at 5.5 MeV/A reactions were measured at the GANIL facility using the INDRA apparatus. This experiment aims to investigate the influence of the neutron enrichment on the decay mechanism of excited nuclei. Data are discussed in comparison with predictions of transition state and Hauser-Feshbach models.


1994 ◽  
Vol 14 (1-3) ◽  
pp. 15-29 ◽  
Author(s):  
Takashi Nagata

The time-of-flight (TOF) spectra of Ar+ and Ar fragments produced in the photodissociation of Arn+ (3 ≦ n ≧ 24) were measured at wavelength around 540 nm. The kinetic-energy and angular distributions of the neutral photofragments were obtained for n = 3, 9 and 24 by a simulation analysis of the measured TOF spectral profiles. The overall aspect of the photodissociation process of Arn+ is deduced from these distributions within the context of trimer ion core model; a linear Ar3+ core is solvated by neutral Ar atoms. For Arn+ with 4 ≦ n ≲ 14, direct dissociation of the Ar3+ chromophoric core gives rise to Ar+ and/or Ar fragments with a high kinetic energy release. For the larger Arn+ (n ≳ 14), the production of high-kinetic-energy fragments is suppressed; “evaporation” of the solvent Ar atoms is instead the dominant channel of photofragmentation.


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