Relativistic proton-impact excitation of hydrogen atom in the presence of intense laser field

2016 ◽  
Vol 94 (7) ◽  
pp. 645-650 ◽  
Author(s):  
E. Hrour ◽  
S. Taj ◽  
A. Chahboune ◽  
B. Manaut

A theoretical treatment, using the first Born approximation, is presented to analyse the results of relativistic laser-assisted proton – hydrogen atom scattering. Specific calculations are carried out for excitation of hydrogen atoms from 1s1/2 to 2s1/2 states by proton impact. We work in an approximation in which the incoming proton may be described by Dirac–Volkov states in the presence of a laser field. Semi-relativistic Darwin wave functions are used to describe the hydrogen atom in its initial and final states, while relativistic, spin, and laser interaction effects are also accounted for. The results presented in this paper show that the differential cross section for this process depends not only upon the energy of the incident proton, but also upon its interaction with the laser field through intensity and frequency.

2020 ◽  
pp. 93-102
Author(s):  
Kishori Yadav ◽  
S.P. Gupta ◽  
J.J. Nakarmi

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.


2020 ◽  
Vol 29 (9) ◽  
pp. 093204
Author(s):  
Yang Song ◽  
Shu Han ◽  
Yu-Jun Yang ◽  
Fu-Ming Guo ◽  
Su-Yu Li

1984 ◽  
Vol 30 (5) ◽  
pp. 2752-2755 ◽  
Author(s):  
H. Bachau ◽  
Robin Shakeshaft

2013 ◽  
Vol 62 (22) ◽  
pp. 223401
Author(s):  
Sun Tian-Miao ◽  
Qi Yue-Ying ◽  
Ye Dan-Dan ◽  
Ning Li-Na

It is shown that the cross-sections given by the customary second Born approximation are not reliable because of the neglect of a large term of the fourth order in the interaction energy. The expression for the cross-section obtained by including only terms to the third order in the interaction energy is employed to calculate the cross-sections for the proton impact excitation of the 2 s state of atomic hydrogen, allowance being made for distortion and polarization due to the 1 s , 2 s and 2 p 0.±1 intermediate states. When polarization is ignored by neglecting all terms involving the 2 p states, excellent agreement is found with the distortion approximation calculation of Bates.


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