Hartree-Slater calculation of the cross section forL-shell ionization of argon by simple heavy charged particles

1975 ◽  
Vol 11 (6) ◽  
pp. 2004-2010 ◽  
Author(s):  
Byung-Ho Choi
Keyword(s):  
Cross Section ◽  
Charged Particles ◽  
Heavy Charged Particles ◽  
The Cross ◽  
Shell Ionization

Energy distribution over the cross section of the track of charged particles having the same linear energy transfer

1973 ◽  
Vol 34 (4) ◽  
pp. 372-373
Author(s):  
I. K. Kalugina ◽  
I. B. Keirim-Markus ◽  
A. K. Savinskii ◽  
I. V. Filyushkin
Keyword(s):  
Energy Transfer ◽  
Energy Distribution ◽  
Cross Section ◽  
Linear Energy Transfer ◽  
Charged Particles ◽  
The Cross

The inner shell ionization of atoms by electron impact

1940 ◽  
Vol 36 (1) ◽  
pp. 43-52 ◽  
Author(s):  
E. H. S. Burhop ◽  
H. S. W. Massey
Keyword(s):  
Experimental Data ◽  
Electron Impact ◽  
Cross Section ◽  
Nickel Silver ◽  
Inner Shell Ionization ◽  
Good For ◽  
The Cross ◽  
Shell Ionization ◽  
Good Agreement

Calculations have been made of the cross-section for ionization of the inner shells of atoms by electron impact in the cases of the K-shells of nickel, silver, mercury and of the three L-shells of silver and mercury.The agreement with experiment is reasonably good for the K-shell ionization, but only fair in the case of the rather meagre experimental data available for the L-shell. The values obtained for the relative ionization in the K- and L-shells are in good agreement with those to be expected from experiment.

Interaction of 14.0 MeV-Neutrons with 12C in Stilbene

1971 ◽  
Vol 26 (2) ◽  
pp. 317-319 ◽  
Author(s):  
H.-U. Fabian
Keyword(s):  
Cross Sections ◽  
Pulse Shape ◽  
Charged Particles ◽  
Pulse Height ◽  
Pulse Height Spectrum ◽  
Pulse Spectrum ◽  
Heavy Charged Particles ◽  
The Cross

AbstractThe pulse height spectrum of all heavy charged particles induced by 14.0 MeV neutrons in a 1" × 1" stilbene scintilla­ tor was measured using a pulse shape discriminator and the associated particle technique. The proton pulse spectrum was subtracted and the remaining alpha-pulse distribution is shown in a diagram. The sum of the cross sections for the reactions 12C (n, n') 3 α and 12C (n, α)9 Be was determined to be σc= (260±20) mb.

Scattering of Non-Relativistic Charged Particles by Electromagnetic Radiation

2017 ◽  
Vol 72 (12) ◽  
pp. 1173-1177
Author(s):  
M. Apostol
Keyword(s):  
Electromagnetic Radiation ◽  
Cross Section ◽  
Charged Particles ◽  
Momentum Conservation ◽  
Potential Scattering ◽  
Photon Absorption ◽  
Focal Region ◽  
Electrons And Ions ◽  
The Cross ◽  
Energy And Momentum

AbstractThe cross-section is computed for non-relativistic charged particles (like electrons and ions) scattered by electromagnetic radiation confined to a finite region (like the focal region of optical laser beams). The cross-section exhibits maxima at scattering angles given by the energy and momentum conservation in multi-photon absorption or emission processes. For convenience, a potential scattering is included and a comparison is made with the well-known Kroll-Watson scattering formula. The scattering process addressed in this paper is distinct from the process dealt with in previous studies, where the scattering is immersed in the radiation field.

Coulomb-deflection effect in inner-shell ionization by heavy charged particles

1980 ◽  
Vol 22 (5) ◽  
pp. 1889-1895 ◽  
Author(s):  
Grzegorz Lapicki ◽  
Roman Laubert ◽  
Werner Brandt
Keyword(s):  
Charged Particles ◽  
Heavy Charged Particles ◽  
Inner Shell Ionization ◽  
Shell Ionization ◽  
Coulomb Deflection

Luminescence of Diatomic Molecules II. Energy Dependence of Collisional Deactivation Cross Sections

1972 ◽  
Vol 27 (5) ◽  
pp. 769-776 ◽  
Author(s):  
F. J. Comes ◽  
F Speier
Keyword(s):  
Excited States ◽  
Cross Section ◽  
Cross Sections ◽  
Charged Particles ◽  
Molecular Ions ◽  
Thermal Velocity ◽  
Vibrational States ◽  
Molecular Gases ◽  
Exponential Law ◽  
The Cross

Abstract Photoionization has been used to produce ions of N2, O2. and CO in definite excited states. Deactivating collisions of these ions with molecular gases were described in paper I, where the cross sections of ions with thermal velocity are given for various electronic and vibrational states. By application of an electric field the charged particles are accelerated yielding information on the influence of the kinetic energy of the collision partners on these deactivating collisions. The cross section is found to follow an exponential law σ ~ E-α, with a varying between 0.34 and 0 41 for the different excited stales of the molecular ions. The observations were carried out for a range of kinetic energies from the thermal energy up to 6 eV maximum. This simple exponential law is followed for kinetic energies up to at least 2 eV. At higher energies slight deviations were found to occur

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