The argon hydrogen–fluoride differential scattering cross section

1989 ◽  
Vol 90 (4) ◽  
pp. 2182-2191 ◽  
Author(s):  
P. F. Vohralik ◽  
R. E. Miller ◽  
R. O. Watts
Keyword(s):  
Cross Section ◽  
Hydrogen Fluoride ◽  
Scattering Cross Section ◽  
Differential Scattering Cross Section ◽  
Scattering Cross

The helium-hydrogen fluoride differential scattering cross-section

1986 ◽  
Vol 58 (4) ◽  
pp. 827-848 ◽  
Author(s):  
C.V. Boughton ◽  
R.E. Miller ◽  
P.F. Vohralik ◽  
R.O. Watts
Keyword(s):  
Cross Section ◽  
Hydrogen Fluoride ◽  
Scattering Cross Section ◽  
Differential Scattering Cross Section ◽  
Scattering Cross

scholarly journals Differential scattering cross section of the dense semiclassical plasma based on the Born method

2020 ◽  
Vol 73 (2) ◽  
pp. 34-40
Author(s):  
E.O. Shalenov ◽  
Zh. Kossymkyzy ◽  
M. Seisembayeva ◽  
R. Masheyeva ◽  
M.N. Jumagulov ◽  
...  
Keyword(s):  
Cross Section ◽  
Scattering Cross Section ◽  
Differential Scattering Cross Section ◽  
Scattering Cross

scholarly journals Elliptically polarized laser assisted elastic electron-hydrogen atom collision and differential scattering cross-section

2020 ◽  
pp. 93-102
Author(s):  
Kishori Yadav ◽  
S.P. Gupta ◽  
J.J. Nakarmi
Keyword(s):  
Hydrogen Atom ◽  
Kinetic Energy ◽  
Cross Section ◽  
Laser Field ◽  
High Energy ◽  
Scattering Cross Section ◽  
Hydrogen Atoms ◽  
Differential Scattering Cross Section ◽  
Scattering Cross ◽  
Cross Section Area

In the present study, we have investigated scattering of an electron by hydrogen atoms in the presence of the elliptical polarized laser field. We have discussed the polarization effect of laser field on hydrogen atom and effect of the resulted polarized potential on differential scattering cross-section is studied. We assume the scattered electrons having kinetic energy (~3000 eV) and laser field of moderate field strength because it is permitted to treat the scattering process in first Born approximation and the scattering electron was described by Volkov wave function. We found that the differential scattering cross-section area increases with the increase of the kinetic energy of the incident electron and there is no effect of changing the value of polarizing angle on the differential cross-section with kinetic energy. We observed that differential scattering cross-section in elliptical polarization in the high energy region depends upon the laser intensity and the incident energy for a linearly polarized field.

Numerical Calculation of Optical Properties of Linear Nano-Graphite Particles

2012 ◽  
Vol 538-541 ◽  
pp. 877-881
Author(s):  
Ya Feng Liu ◽  
Chao Jun Huang
Keyword(s):  
Cross Section ◽  
Incident Angle ◽  
Incident Light ◽  
Efficiency Factor ◽  
Scattering Cross Section ◽  
Differential Scattering Cross Section ◽  
Extinction Efficiency ◽  
Graphite Particles ◽  
Scattering Cross ◽  
Variation Tendency

Using the discrete dipole approximation method, the absorption, scattering, extinction efficiency factor and differential scattering cross section of four kinds of nano-graphite particles under different incident angle are numerical calculated, the result shown that the value of the absorption, scattering, extinction efficiency factor and differential scattering cross section of linear nano-graphite particles are symmetric on the incident angle. There are the same variation tendency of absorption and extinction efficiency factor changed with the incident angle, when the incident light parallel with the linear nano-graphite particles, both the absorption and extinction are the strongest, and when the incident light perpendicular the linear nano-graphite particles, both the absorption and extinction are the weakest. The variation tendency of scattering efficiency factor changed with incident angle depended on the number of single graphite and the arrangement of linear nano-graphite particles. The value of differential scattering cross section is the smallest while the incident light parallel with the linear nano-graphite particles, however, the biggest while the incident light perpendicular the linear nano-graphite particles.

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