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
Author(s):  
Tamotsu Ohno

The energy distribution in an electron; beam from an electron gun provided with a biased Wehnelt cylinder was measured by a retarding potential analyser. All the measurements were carried out with a beam of small angular divergence (<3xl0-4 rad) to eliminate the apparent increase of energy width as pointed out by Ichinokawa.The cross section of the beam from a gun with a tungsten hairpin cathode varies as shown in Fig.1a with the bias voltage Vg. The central part of the beam was analysed. An example of the integral curve as well as the energy spectrum is shown in Fig.2. The integral width of the spectrum ΔEi varies with Vg as shown in Fig.1b The width ΔEi is smaller than the Maxwellian width near the cut-off. As |Vg| is decreased, ΔEi increases beyond the Maxwellian width, reaches a maximum and then decreases. Note that the cross section of the beam enlarges with decreasing |Vg|.


1996 ◽  
Vol 145 (3) ◽  
pp. 251 ◽  
Author(s):  
Li X. Zhu ◽  
Charles A. Waldren ◽  
Diane Vannais ◽  
Tom K. Hei

1983 ◽  
Vol 26 (2) ◽  
pp. 109-111 ◽  
Author(s):  
N. A. Kolhanovskaya ◽  
A. F. Kotyuk ◽  
A. M. Raitsin

1988 ◽  
Vol 9 (7) ◽  
pp. 1233-1236 ◽  
Author(s):  
Tom K. Hei ◽  
David J. Chen ◽  
David J. Brenner ◽  
Eric J. Hall

2017 ◽  
Vol 72 (12) ◽  
pp. 1173-1177
Author(s):  
M. Apostol

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.


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