1981
DOI: 10.1103/physreva.24.2473
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Extension of the Schwinger variational principle beyond the static-exchange approximation

Abstract: We propose a new variational principle for scattering theory which extends the Schwinger variational principle beyond the static-exchange approximation and to inelastic scattering. Application of this formulation to the scattering of electrons by hydrogen atoms at energies below k' = 0.64 demonstrates the rapid convergence of the phase shift with respect to the number of basis functions for both the open-and closed-channel orbitals. Furthermore, we show that the convergence of the phase shift with respect to t… Show more

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Cited by 353 publications
(201 citation statements)
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References 31 publications
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“…The first electronic excitation energy of CH 3 OH is found to be 8.55 eV using the configuration interaction (CI) model, which agrees well with the calculated value of 8.53 eV reported by Vinodkumar et al [12], albeit higher compared to the theoretical value of 6.76 eV reported by Bouchiha et al [3] and the experimental value of 6.5 eV reported by Knoop et al [19]. The present dipole moment is 2.28 D, which is slightly higher compared to the theoretical value of 1.97 D [3] The most popular methodologies employed for low-energy electron collision calculations are the Kohn variational method [20,21], the Schwinger variational method [22][23][24], and the R-matrix method, of which the R matrix is the most widely used. The underlying idea behind the R-matrix method relies on the division of configuration space into two spatial regions, namely, the inner region and the outer region.…”
Section: A Target Model Used For Low-energy Calculationscontrasting
confidence: 43%
“…The first electronic excitation energy of CH 3 OH is found to be 8.55 eV using the configuration interaction (CI) model, which agrees well with the calculated value of 8.53 eV reported by Vinodkumar et al [12], albeit higher compared to the theoretical value of 6.76 eV reported by Bouchiha et al [3] and the experimental value of 6.5 eV reported by Knoop et al [19]. The present dipole moment is 2.28 D, which is slightly higher compared to the theoretical value of 1.97 D [3] The most popular methodologies employed for low-energy electron collision calculations are the Kohn variational method [20,21], the Schwinger variational method [22][23][24], and the R-matrix method, of which the R matrix is the most widely used. The underlying idea behind the R-matrix method relies on the division of configuration space into two spatial regions, namely, the inner region and the outer region.…”
Section: A Target Model Used For Low-energy Calculationscontrasting
confidence: 43%
“…Cross sections for elastic electron scattering by and electron-impact excitation of CHF 3 were computed using the Schwinger multichannel ͑SMC͒ method 7,8 as implemented for parallel computers. 9,10 Details of the method may be found in the references given.…”
Section: A Computational Methodsmentioning
confidence: 99%
“…Electron-scattering calculations were carried out at the optimized geometry using a massively parallel implementation of the Schwinger multichannel (SMC) variational method [22][23][24]. The one-electron space used in the calculations was constructed along the same lines as that used in earlier work on ethylene [25,26].…”
Section: B Theorymentioning
confidence: 99%