Electron capture cross sections by different atoms based on the perturbation theory

Authors

  • E.O. Shalenov Al-Farabi Kazakh National University, Institute of Experimental and Theoretical Physics, Kazakhstan, Almaty
  • M. Seisembayeva Al-Farabi Kazakh National University, Institute of Experimental and Theoretical Physics, Kazakhstan, Almaty
  • K.N. Dzhumagulova Al-Farabi Kazakh National University, Institute of Experimental and Theoretical Physics, Kazakhstan, Almaty

DOI:

https://doi.org/10.26577/rcph-2019-i2-12

Keywords:

capture cross section, effective interaction potential, semiclassical plasma, electron capture, capture radius

Abstract

In this work the results of numerical calculation of the electron capture radius in partially ionized plasma are presented. The effective interaction potential was chosen as the electron-atom interaction, which takes into account the screening effect at large distances and the diffraction effect on small distances. The results on the electron capture radius for different chemical elements were obtained based on the perturbation theory. Also, on the basis of the effective interaction potential of an electron with an atom of a nonideal semiclassical plasma, the capture time and the differential capture cross section for different chemical elements are investigated. The results showed that for large values of polarizability coefficient the electron capture radius increases. On the basis of perturbation theory the interaction time between the electron and other atoms was calculated. Studies have shown that with increasing polarizability coefficient the differential capture cross section rises. For this goal the Bohr–Lindhard method has been applied to obtain the electron capture cross section.

References

1 T.S. Ramazanov, K.N. Dzhumagulova, et al, Physics of Plasmas 12, 092702 (2015).

2 E.O. Shalenov et al., Proc. of the 45th EPS Conference on Plasma Physics, 561 (2018).

3 K.N. Dzhumagulova, E.O. Shalenov and G.L. Gabdullina, Rec. Contr. Phys. 3(54), 18-24 (2015). (in Russ).

4 E.O. Shalenov et. al., Intern. J of Mathematics and Physics 7, 131 (2016).

5 E.O. Shalenov, K.N. Dzhumagulova and T.S. Ramazanov, Rec. Contr. Phys. 62, 26-33 (2017). (in Russ).

6 K.N. Dzhumagulova, et al, Physics of Plasmas 20, 042702 (2013).

7 K.N. Dzhumagulova, , et al, Physics of Plasmas 22, 082120 (2015).

8 K.N. Dzhumagulova et. al., Contrib. Plasma Physics 57, 230 (2015).

9 E.O. Shalenov, K.N. Dzhumagulova and T.S. Ramazanov, Physics of Plasmas 24, 012101 (2017).

10 E.O. Shalenov et. al., Contrib. Plasma Physics 57, 486 (2017).

11 E.O. Shalenov et. al., Physics of Plasmas 25, 082706 (2018).

12 T.S. Ramazanov, K.N. Dzhumagulova and A.Z. Akbarov, J. Phys. A: Math. Gen. Plasmas 39, 4335 (2006).

13 T.S. Ramazanov et. al., Contr. Plasma Physics 47, 262 (2007).

14 T.S. Ramazanov et. al., PLTP (Kiev: Naukova dumka, 2004), p. 5.9.103.

15 T.F. Drukarev, Teorija stolknovenij jelektronov s atomami (Мoscow: Fizmatgiz, 1963), p. 37. (in Russ).

16 T.S. Ramazanov et. al., Contr. Plasma Physics 47, 262 (2007).

17 K.N. Dzhumagulova et. al, 15th International Conference on the Physics of Non-Ideal Plasmas, Book of abstracts, 116 (2015).

18 T.S. Ramazanov, K.N. Dzhumagulova, A.Zh. Akbarov, and M.T. Gabdullin, PLTP (Kiev, Naukova dumka, 2004), 5.9.10 р.

19 E.O. Shalenov et al., Proc. of the 45th EPS Conf. on Plasma Physics, 557 (2018).

20 K.N. Dzhumagulova, M.M. Seisembayeva, et al, Rec. Contr. Phys. 4(55), 12-19 (2015). (in Russ).

21 M.M. Seisembayeva, K.N. Dzhumagulova and T.S. Ramazanov, Nukleonika 61, 201 (2016).

22 D.-H. Ki and Y.-D., Jour. Chem. Phys., 137, 094310 (2012).

23 I. Ben-Itzhak, A. Jaint and O.L. Weaver, J. Phys. B. 26, 1711 (1993).

24 Y.-D. Jung and M. Akbari-Moghanjoughi, Physics of Plasmas 21, 032108 (2014).

25 Y.-D. Jung, Physics of Plasmas 4, 16 (1997).

26 D.A. Brandt, Nucl. Instrum. Methods 214, 93 (1983).

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Published

2019-06-24