Direct interaction theory of inelastic scattering. Part I

1957 ◽  
Vol 2 (5) ◽  
pp. 471-498 ◽  
Author(s):  
Carl A Levinson ◽  
Manoj K Banerjee
1957 ◽  
Vol 2 (5) ◽  
pp. 499-524 ◽  
Author(s):  
Manoj K Banerjee ◽  
Carl A Levinson

1958 ◽  
Vol 3 (1) ◽  
pp. 67-90 ◽  
Author(s):  
Carl A Levinson ◽  
Manoj K Banerjee

Physica ◽  
1956 ◽  
Vol 22 (6-12) ◽  
pp. 1163-1164
Author(s):  
N.C. Francis ◽  
P.F. Zweifel

1961 ◽  
Vol 39 (7) ◽  
pp. 957-966 ◽  
Author(s):  
R. L. Clarke

The spectrum and absolute yield of neutrons resulting from 14-Mev neutrons incident on natural uranium was observed at 90°± 16 to the incident neutron beam by a time-of-flight method. Further observations of the spectrum from 9 to 13.5 Mev were made for scattering angles at 30° and 60°. In addition to the expected neutrons resulting from evaporation and fission, strong evidence is seen for direct interaction inelastic scattering. The (n,n′) cross section is estimated to be 150 ± 70 millibarns.


2017 ◽  
Vol 35 (3) ◽  
pp. 683-690 ◽  
Author(s):  
Rudolf A. Treumann ◽  
Wolfgang Baumjohann

Abstract. Statistical plasma theory far from thermal equilibrium is subject to Liouville's equation, which is at the base of the BBGKY hierarchical approach to plasma kinetic theory, from which, in the absence of collisions, Vlasov's equation follows. It is also at the base of Klimontovich's approach which includes single-particle effects like spontaneous emission. All these theories have been applied to plasmas with admirable success even though they suffer from a fundamental omission in their use of the electrodynamic equations in the description of the highly dynamic interactions in many-particle conglomerations. In the following we extend this theory to taking into account that the interaction between particles separated from each other at a distance requires the transport of information. Action needs to be transported and thus, in the spirit of the direct-interaction theory as developed by Wheeler and Feynman (1945), requires time. This is done by reference to the retarded potentials. We derive the fundamental causal Liouville equation for the phase space density of a system composed of a very large number of charged particles. Applying the approach of Klimontovich (1967), we obtain the retarded time evolution equation of the one-particle distribution function in plasmas, which replaces Klimontovich's equation in cases when the direct-interaction effects have to be taken into account. This becomes important in all systems where the distance between two points |Δq| ∼ ct is comparable to the product of observation time and light velocity, a situation which is typical in cosmic physics and astrophysics.


1959 ◽  
Vol 114 (5) ◽  
pp. 1297-1311 ◽  
Author(s):  
Norman K. Glendenning

1968 ◽  
Vol 46 (20) ◽  
pp. 3157-3170
Author(s):  
M. K. Dewanjee ◽  
G. B. Saha ◽  
L. Yaffe

Thick-target recoil experiments were performed to study (p,pn) reactions induced in 65Cu and 197Au in the energy range of 20–85 MeV and the average ranges projected in the forward, backward, and perpendicular directions were determined. Recoil parameters have been calculated to show approximately the amount of energy transfer and their energy dependence. The average range results have been compared with statistical theory, cascade–evaporation (85 MeV only), and inelastic scattering model calculations. The statistical calculations show reasonable agreement up to 30–40 MeV. However, the calculated projected range values, based on the cascade–evaporation and the inelastic scattering models, are consistently lower than the measured values. The analyses of the projected range values support the prevalent view that at low energies (~ 30–35 MeV), the compound nucleus mechanism is predominant and at higher energies, the direct interaction mechanism makes a major contribution.


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