1992
DOI: 10.1016/0370-1573(92)90161-r
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Kramers electrodynamics and electron-atomic radiative-collisional processes

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Cited by 58 publications
(26 citation statements)
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“…The latter is based on the applicability of classical approximation to the Thomas-Fermi (TF) statistical potential. This was demonstrated in calculations of bremsstrahlung spectra [16] on multielectrons systems, which are in excellent agreement with quantum calculations of corresponding effects. The application of the Fermi method of equivalent photons [17] allows the consideration of the excitation processes in atoms as photoabsorption of the equivalent photon flux.…”
Section: Introductionsupporting
confidence: 60%
See 1 more Smart Citation
“…The latter is based on the applicability of classical approximation to the Thomas-Fermi (TF) statistical potential. This was demonstrated in calculations of bremsstrahlung spectra [16] on multielectrons systems, which are in excellent agreement with quantum calculations of corresponding effects. The application of the Fermi method of equivalent photons [17] allows the consideration of the excitation processes in atoms as photoabsorption of the equivalent photon flux.…”
Section: Introductionsupporting
confidence: 60%
“…is the Gaunt-factor, that describes the curvature of electron trajectory in the given potential of an ion with the charge zi and the charge of nuclei Z in the Coulomb approximation [13][14][15][16]. Now we multiply the photoionization cross-section by the number of EQP (4) …”
Section: Ionization Cross-sections and Ratesmentioning
confidence: 99%
“…According to the quasi-classical theory of radiative transitions [33], the emission of photons with the energy k by an electron is most effective in the turning point r 0 of the classical trajectory for which the angular electron velocity is close to k. Therefore, the distance r 0 in Equation (21) may be determined as a root of the equation, which is written in atomic units as follows:…”
Section: Model Used In Calculationsmentioning
confidence: 99%
“…³áAE ÉÇ ÑÕÐÑÔâÕÔâ ÖÒÑÏâÐÖÕÞÇ ÕÂÏ ÒÓËÏÇÓÞ "AEÇ×ÇÐÑÏÇÐÑÎÑÅËÊÂÙËË" ÒÇÓÄÑÅÑ ÒÑÔÕÖÎÂÕ ¢ÑÓÂ,  ÕÂÍÉÇ "ÓÂAEËÑÂÍÕËÄÐÑÌ ÂÐÂÎÑÅËË" ¿ÌÐÛÕÇÌРAEÎâ ÔÒÑÐÕÂÐÐÑÅÑ ËÊÎÖÚÇÐËâ. ¦ÜÇ ÑAEËÐ ÒÓËÏÇÓ, ÓÂÔÔÏÑÕÓÇÐ-ÐÞÌ Ä [8], ÂÐÂÎËÕËÚÇÔÍË AEÇÏÑÐÔÕÓËÓÖÇÕ ÒÓËÃÎËÉÇÐÐÖá ÄÊÂËÏÐÖá àÍÄËÄÂÎÇÐÕÐÑÔÕß "×ÇÐÑÏÇÐÑÎÑÅËÚÇÔÍÑÅÑ" ÖÓÂÄÐÇÐËâ " ho E 1 À E 2 (ÄÕÑÓÑÌ ÒÑÔÕÖÎÂÕ ¢ÑÓÂ) Ë "ÏËÍ-ÓÑÔÍÑÒËÚÇÔÍÑÅÑ" ÔÑÑÕÐÑÛÇÐËâ " ho % E ³ÒËÔÑÍ ÎËÕÇÓÂÕÖÓÞ…”
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