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Triple differntial cross section for electron impact ionization of hydrogen atom
Atomic Physics · Submitted 23 May 2019
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The electron impact ionization of atomic hydrogen is calculated for incident elrctron energy 76.46 eV.
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The abstract, sentence by sentence
The electron impact ionization of atomic hydrogen is calculated for incident elrctron energy 76.46 eV. The Hartree-Fock approximation is used to calculate the initial state which includes both bound and continum wave functions. The final state continuum electron wave functions are obtained in the potential of hydrogen ion. The interaction between the two final state continuum electrons is approximated with the screening potential determined variationally.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The electron impact ionization of atomic hydrogen is calculated for incident elrctron energy 76.46 eV. | contribution 0.89 | 0.89 | 0.07 | asserted 1.00 |
| s1 | The Hartree-Fock approximation is used to calculate the initial state which includes both bound and continum wave functions. | method 1.00 | 0.83 | 0.03 | asserted 1.00 |
| s2 | The final state continuum electron wave functions are obtained in the potential of hydrogen ion. | method 1.00 | 0.84 | 0.03 | asserted 1.00 |
| s3 | The interaction between the two final state continuum electrons is approximated with the screening potential determined variationally. | method 0.99 | 0.85 | 0.05 | asserted 1.00 |
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Original abstract
The electron impact ionization of atomic hydrogen is calculated for incident elrctron energy 76.46 eV. The Hartree-Fock approximation is used to calculate the initial state which includes both bound and continum wave functions. The final state continuum electron wave functions are obtained in the potential of hydrogen ion. The interaction between the two final state continuum electrons is approximated with the screening potential determined variationally.
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