Times of emission of K x rays from U235 fission fragments of known mass

1974 ◽  
Vol 45 (5) ◽  
pp. 2327-2335 ◽  
Author(s):  
R. A. Lerche ◽  
B. W. Wehring ◽  
M. E. Wyman
1964 ◽  
Vol 55 ◽  
pp. 249-256 ◽  
Author(s):  
V.F. Apalin ◽  
Yu.N. Gritsyuk ◽  
I.E. Kutikov ◽  
V.I. Lebedev ◽  
L.A. Mikaelyan

Author(s):  
K Butler-Moore ◽  
R Aryaeinejad ◽  
J.D Cole ◽  
Y Dardenne ◽  
R.C Greenwood ◽  
...  
Keyword(s):  
X Rays ◽  

1986 ◽  
Vol 64 (6) ◽  
pp. 665-670 ◽  
Author(s):  
S. Ahmad ◽  
O. Häusser ◽  
J. A. Macdonald ◽  
B. H. Olaniyi ◽  
A. Olin ◽  
...  

Muon-induced prompt and delayed fission yields in 235U and 238U have been measured. A coincidence with the muonic uranium Kα X-rays was used to identify the muon stop in the target. The experimental absolute fission yields per muon stop were 0.142 ± 0.023 for 235U and 0.068 ± 0.013 for 238U. The disappearance rate of muons from the 1s state of muonic uranium has also been measured in the fission mode. Muon-induced fission lifetimes were 71.6 ± 0.6 ns for 235U and 77.2 ± 0.4 ns for 238U. No evidence for a short-lifetime fission – isomer component was found. Comparison of lifetime results with previously measured values in the electron, gamma, and neutron decay modes indicated that the systematic discrepancies could be explained by muon capture on fission fragments produced from prompt fission.


1962 ◽  
Vol 40 (8) ◽  
pp. 943-953 ◽  
Author(s):  
H. Farrar ◽  
R. H. Tomlinson

Recent measurements of the cumulative yields of essentially all the mass chains in the thermal neutron fission of U235 have enabled a detailed examination of the fine structure in the mass–yield curve. It has been found that most of the structure results from a slowly changing neutron yield as a function of the mass of the primary fission fragments.


1965 ◽  
Vol 19 (3) ◽  
pp. 1156-1161
Author(s):  
F. Nasyrov ◽  
A. A. Rostovtsev ◽  
Yu. I. Il'in ◽  
S. V. Linev

1966 ◽  
Vol 20 (6) ◽  
pp. 536-540 ◽  
Author(s):  
F. Nasyrov ◽  
S. V. Linev

1994 ◽  
Vol 144 ◽  
pp. 82
Author(s):  
E. Hildner

AbstractOver the last twenty years, orbiting coronagraphs have vastly increased the amount of observational material for the whitelight corona. Spanning almost two solar cycles, and augmented by ground-based K-coronameter, emission-line, and eclipse observations, these data allow us to assess,inter alia: the typical and atypical behavior of the corona; how the corona evolves on time scales from minutes to a decade; and (in some respects) the relation between photospheric, coronal, and interplanetary features. This talk will review recent results on these three topics. A remark or two will attempt to relate the whitelight corona between 1.5 and 6 R⊙to the corona seen at lower altitudes in soft X-rays (e.g., with Yohkoh). The whitelight emission depends only on integrated electron density independent of temperature, whereas the soft X-ray emission depends upon the integral of electron density squared times a temperature function. The properties of coronal mass ejections (CMEs) will be reviewed briefly and their relationships to other solar and interplanetary phenomena will be noted.


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