1981
DOI: 10.1088/0022-3700/14/23/004
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Comments on the triple differential ionisation cross sections in the second Born approximation

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Cited by 7 publications
(11 citation statements)
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“…Recently, Dal Cappello et al [7] have shown that the second Born approximation works very well for the ionization of atomic hydrogen for an incident energy of 250 eV and an energy of 5 eV for the ejected electron but completely fails for higher values of the energy of the ejected electrons (50 eV). This result was also found by Pathak and Srivastava [8] who only used the closure approximation. In our studies, the incident electron is described by a plane wave.…”
Section: Introductionsupporting
confidence: 84%
See 1 more Smart Citation
“…Recently, Dal Cappello et al [7] have shown that the second Born approximation works very well for the ionization of atomic hydrogen for an incident energy of 250 eV and an energy of 5 eV for the ejected electron but completely fails for higher values of the energy of the ejected electrons (50 eV). This result was also found by Pathak and Srivastava [8] who only used the closure approximation. In our studies, the incident electron is described by a plane wave.…”
Section: Introductionsupporting
confidence: 84%
“…We also study in greater detail the closure approximation. We have known for a long time that the closure approximation works very well for low energy for the ejected electrons [7,9,21,22], but fails for higher energies [7,8]. We decide to investigate this issue mostly in the highest possible energy regime 50 eV of the ejected electron.…”
Section: Introductionmentioning
confidence: 99%
“…From this good agreement between the two theories (CDW-EIS and CCC) they conclude that the experimental data of Ehrhardt et al (1985Ehrhardt et al ( , 1986 . These experiments are interesting because Pathak and Srivastava (1981) conclude that the second Born approximation is not able to bring about a general improvement in the values of the TDCS over the first Born results. These authors use the closure approximation with a high average excitation energy w =1 au.…”
Section: Results and Discussion A) Ionization Of Atomic Hydrogen By Ementioning
confidence: 93%
“…We only notice small differences between the two calculations and find results close to those of Byron et al (1982): the first and second Born triple differential cross sections differ by only 17% at the binary peak, with the second Born result being smaller than the first Born result (as in the case of atomic hydrogen).We also find that the ratio of the binary peak to the recoil peak is reduced from the first Born value of 8.43 to the second Born value of 5.63 in better agreement with experiment. Thus, as written by Byron et al (1982), the results of Pathak and Srivastava (1981) in this case are incorrect.…”
Section: C) Single Ionization Of Helium By Electronsmentioning
confidence: 97%
“…Pathak and Srivastava [32] used the second Born approximation for the ionization of atomic hydrogen and compared their results to the first (e, 2e) experiments of Weigold et al [33], Then they also made calculations for the ionization of helium by using the closure approximation and compared their results to those of Ehrhardt et al [34], Byron et al [35] also calculated TDCSs for the ionization of helium by using the closure approximation and found results which disagreed with those of Pathak and Srivastava [32], Later on, Byron et al [36] applied the second Born approximation by using very few discrete states as intermediate states and by taking into account the closure approximation and adding the contribution of the third Born approximation calculated with the Glauber approximation. It was found that the second Born PACS number(s): 34.50.Rk, 34.80.Dp, 34.50.Fa calculation plays a crucial role in understanding the (e, 2e) process.…”
Section: Introductionmentioning
confidence: 99%