scholarly journals SENSING THE OPTIMAL PLASMA PARAMETERS FOR X-RAY LASING: CALCULATION OF ELECTRON-COLLISION EXCITATION CROSS-SECTIONS FOR Ar-LIKE PLASMA IONS

2014 ◽  
Vol 3 (1) ◽  
pp. 18-22
Author(s):  
E. P. Gurnitskaya ◽  
D. A. Korchevsky ◽  
A. V. Loboda
1995 ◽  
Vol 48 (3) ◽  
pp. 357 ◽  
Author(s):  
Y Nakamura

The drift velocity and longitudinal diffusion coefficient of electrons in 0�2503% and 1� 97% C02-Ar mixtures were measured for 0�03 ~ E/N ~ 20 Td. The measured electron swarm parameters in the mixtures were used to derive a set of consistent vibrational excitation cross sections for the C02 molecule. Analysis of electron swarms in pure C02 using the present vibrational excitation cross sections was also carried out in order to determine a new momentum transfer cross section for the C02 molecule.


2005 ◽  
Vol 104 (4) ◽  
pp. 562-569 ◽  
Author(s):  
Alexander V. Glushkov ◽  
Sergey V. Ambrosov ◽  
Andrey V. Loboda ◽  
Elena P. Gurnitskaya ◽  
Georgy P. Prepelitsa

2021 ◽  
Vol 914 (1) ◽  
pp. 34
Author(s):  
Chintan Shah ◽  
Natalie Hell ◽  
Antonia Hubbard ◽  
Ming Feng Gu ◽  
Michael J. MacDonald ◽  
...  

2007 ◽  
Vol 4 (2) ◽  
pp. 9-13
Author(s):  
A. V. Glushkov ◽  
O. Yu. Khetselius ◽  
E. P. Gurnitskaya ◽  
D. A. Korchevsky ◽  
A. V. Loboda ◽  
...  

Author(s):  
R.F. Egerton

SIGMAL is a short (∼ 100-line) Fortran program designed to rapidly compute cross-sections for L-shell ionization, particularly the partial crosssections required in quantitative electron energy-loss microanalysis. The program is based on a hydrogenic model, the L1 and L23 subshells being represented by scaled Coulombic wave functions, which allows the generalized oscillator strength (GOS) to be expressed analytically. In this basic form, the model predicts too large a cross-section at energies near to the ionization edge (see Fig. 1), due mainly to the fact that the screening effect of the atomic electrons is assumed constant over the L-shell region. This can be remedied by applying an energy-dependent correction to the GOS or to the effective nuclear charge, resulting in much closer agreement with experimental X-ray absorption data and with more sophisticated calculations (see Fig. 1 ).


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