Measurements of fragment mass, charge and kinetic energy distributions in thermal neutron fission of 235U with a back-to-back ΔE-E detector system

1983 ◽  
Vol 410 (3) ◽  
pp. 458-474 ◽  
Author(s):  
Rekha Govil ◽  
S.S. Kapoor ◽  
D.M. Nadkarni ◽  
S.R.S. Murthy ◽  
P.N.Rama Rao
1977 ◽  
Vol 16 (2) ◽  
pp. 716-720 ◽  
Author(s):  
A. Ramaswami ◽  
Satya Prakash ◽  
S. B. Manohar ◽  
S. P. Dange ◽  
P. P. Venkatesan ◽  
...  

1971 ◽  
Vol 24 (4) ◽  
pp. 821 ◽  
Author(s):  
JW Boldeman ◽  
AR de L Musgrove ◽  
RL Walsh

Measurements have been made of prompt neutron emission in the thermal neutron fission of 235 U and the mean neutron emission per fragment has been obtained for particular values of the fragment mass and total kinetic energy. A direct neutron counting method was employed and a comparison is made with data from previous experiments of this type.


1994 ◽  
Vol 213-214 ◽  
pp. 417-419
Author(s):  
I. Nishinaka ◽  
M. Tanikawa ◽  
S. Miyamoto ◽  
K. Sueki ◽  
H. Nakahara ◽  
...  

1962 ◽  
Vol 40 (11) ◽  
pp. 1626-1663 ◽  
Author(s):  
J. C. D. Milton ◽  
J. S. Fraser

The prompt mass and kinetic energy distributions resulting from the thermal neutron fission of U233, U235, and Pu239 have been reinvestigated using time-of-flight methods to measure simultaneously the velocities of the fragment pairs. A new feature shown by the present work is the existence of fine structure in the prompt mass yields. This fine structure is most pronounced at high total kinetic energies where the fragments have little excitation energy and may be associated with irregularities in the energy release as a function of mass. The fine structure is most noticeable in U235 and least in Pu239; the fragments of U235 have the lowest average excitation and those of Pu239, the highest. Another feature, which is confirmed by this work, is the large drop in total kinetic energy when the fragments are near symmetry. This decrease is about 35 Mev and is consistent either with a picture in which the nucleus with 50 protons is especially preferred or with one in which fragments at symmetric fission have an abnormally high excitation energy and a consequent large number of neutrons. The mean kinetic energies for thermal neutron fission of U233, U235, and Pu239 were found to be 167.6, 168.3, and 175.0 Mev with an error of ± 1.7 Mev.


1973 ◽  
Vol 8 (3) ◽  
pp. 1018-1022 ◽  
Author(s):  
Frances Pleasonton ◽  
Robert L. Ferguson ◽  
Franz Plasil ◽  
C. E. Bemis

1987 ◽  
Vol 98 (5) ◽  
pp. 643-656 ◽  
Author(s):  
S. Ló Nigro ◽  
S. Aiello ◽  
G. Lanzanò ◽  
C. Milone ◽  
A. Pagano ◽  
...  

1972 ◽  
Vol 34 (9) ◽  
pp. 2685-2697 ◽  
Author(s):  
Satya Prakash ◽  
S.B. Manohar ◽  
S.P. Dange ◽  
A. Ramaswami ◽  
M.V. Ramaniah

1959 ◽  
Vol 37 (8) ◽  
pp. 916-925 ◽  
Author(s):  
H. R. Fickel ◽  
R. H. Tomlinson

The relative cumulative yields of 19 light mass fragments of rubidium, strontium, yttrium, zirconium, molybdenum, and ruthenium formed in the thermal neutron fission of Pu239 have been determined with a mass spectrometer using the isotope dilution technique.The yields of the fission product isotopes of these elements, together with the previously published relative yields of three krypton isotopes, have made possible the determination of the absolute yields of 22 light fragment mass chains.


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