1989
DOI: 10.1007/bf01436585
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Electron impact ionization of atomic hydrogen

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1989
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Cited by 37 publications
(46 citation statements)
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“…10 On the other hand, the TDCS's for the 012 = IT case given by calculations using the effective-charge approximation [2,10,[12][13][14]171 are independent of the excess energy in the Ex + 0 limit. This threshold behavior can be verified by analyzing the wave functions used in such calculations.…”
Section: Wannier-peterkop-rau Threshold Lawmentioning
confidence: 99%
See 1 more Smart Citation
“…10 On the other hand, the TDCS's for the 012 = IT case given by calculations using the effective-charge approximation [2,10,[12][13][14]171 are independent of the excess energy in the Ex + 0 limit. This threshold behavior can be verified by analyzing the wave functions used in such calculations.…”
Section: Wannier-peterkop-rau Threshold Lawmentioning
confidence: 99%
“…Recently we have presented distorted-wave calculations of the triply differential cross sections for electron impact ionization of H, He, Ne, Ar, Kr, Xe, Li, and Mg for final-state electrons departing in opposite directions (€Il2 = n) and sharing between 0.5 eV and 4 eV excess energy (Ex) [14]. The results for H and the rare gases were shown [1,2] to agree well with the available relative experimental measurements [5-81. In particular, they provided an interpretation of the observed target dependence of the electron angular distributions for H and He targets [6] in terms of short-range effects on the s-wave phase shifts of both incident and final-state continuum electrons [I-21.…”
Section: Introductionmentioning
confidence: 99%
“…0 in the WPR theory owing to the predicted rapid narrowing of the width of the distribution with respect to u 12 in the region of u 12 p. The DPW results, however, which employ an effective screening approximation [23][24][25], are independent of E ex as E ex ! 0.…”
mentioning
confidence: 99%
“…The final-state wave function C 2 f is also an expansion in independent-electron states for each of the two continuum electrons, in which their orbital and spin angular momenta are coupled to partial waves characterized by L and S, which are the total orbital and spin angular momenta of the system. The major approximation to C 2 f is the replacement of the exact Coulomb interaction between the two continuum electrons by a variationally determined screening potential [23][24][25]. The DPW approach thus treats distortion, nonlocal exchange interactions, both singlet and triplet partial waves, and mutual screening interactions using effective charges which satisfy proper asymptotic boundary conditions.…”
mentioning
confidence: 99%
“…However, we have ignored such interchannel coupling and treat the channels designated by L and S as uncoupled. The major approximation to Ψ f -in our calculation is our replacement of the exact Coulomb interaction between the two continuum electrons by a variationally determined screening potential [20][21][22]. Further details on the DPW approach are presented in [4,23].…”
mentioning
confidence: 99%