The Time-Dependent Hartree-Fock Formalism of the Double Excited States of the Helium Atom

Article Preview

Abstract:

The solution of the time-dependent Schrödinger equation for the helium atom in double excited states using the time-dependent Hartree-Fock (TDHF) equation is outlined in this work. Schwartz interpolation is used to derive grid representations that are particularly suitable for problems involving the Coulomb potential. This method allows a non-uniform spatial discretization of grid and provides an accurate description of the excited states, eigenvalues and wave functions with a few numbers of grid points. We have introduced the solution using the Coulomb Wave Function Discrete Variable Representation (CWDVR) which is an economical and promising step towards a more efficient treatment of many-electron systems. The equation is transformed into a diffusion type equation by an imaginary-time evolution method and the solution is obtained numerically. The asymptotic solution of these equations leads to definite energy double excited states. We have shown that the calculated electronic energies for the helium atom agree well with the best available values.

You might also be interested in these eBooks

Info:

Periodical:

Pages:

3-10

Citation:

Online since:

November 2025

Export:

Price:

Permissions CCC:

Permissions PLS:

Сopyright:

© 2025 Trans Tech Publications Ltd. All Rights Reserved

Share:

Citation:

* - Corresponding Author

[1] S. Esposito and A. Naddeo, Majorana solutions to the two-electron problem, Found. Phys. 42 (2012), 1586–1608.

DOI: 10.1007/s10701-012-9685-1

Google Scholar

[2] D. J. Griffiths, Introduction to Quantum Mechanics, second ed., Pearson Prentice Hall, Upper Saddle River, New Jersey, 2005.

Google Scholar

[3] S. Koonin and D. Meredith, Computational Physics, Perseus Books, Reading, Massachusetts, 1998).

Google Scholar

[4] A. S. Dickinson and P. R. Certain, Calculation of Matrix Elements for One‐Dimensional Quantum‐Mechanical Problems, J. Chem. Phys. 49 (1968), 4209.

DOI: 10.1063/1.1670738

Google Scholar

[5] J. V. Lill, G. A. Parker, and J. C. Light, Discrete variable representations and sudden models in quantum scattering theory, Chem. Phys. Lett. 89 (1982), 483.

DOI: 10.1016/0009-2614(82)83051-0

Google Scholar

[6] J. Light, I. Hamilton, and J. Lill, Generalized discrete variable approximation in quantum mechanics, J. Chem. Phys. 82 (1985) 1400.

DOI: 10.1063/1.448462

Google Scholar

[7] Z. Bačić and J. Light, Highly excited vibrational levels of "floppy" triatomic molecules: A discrete variable representation—Distributed Gaussian basis approach, J. Chem. Phys. 85 (1986), 4594.

DOI: 10.1063/1.451824

Google Scholar

[8] Z. Bačić and J. Light, Accurate localized and delocalized vibrational states of HCN/HNC, J. Chem. Phys. 86 (1987), 3065.

DOI: 10.1063/1.452017

Google Scholar

[9] R. M. Whitnell and J. Light, Efficient pointwise representations for vibrational wave functions: Eigenfunctions of H+3, J. Chem. Phys. 90 (1989), 1774.

DOI: 10.1063/1.456071

Google Scholar

[10] S. E. Choi and J. Light, Determination of the bound and quasibound states of ar–hcl van der Waals complex: discrete variable representation method, J. Chem. Phys. 92 (1990), 2129.

DOI: 10.1063/1.458004

Google Scholar

[11] D. O. Harris, G. G. Engerholm, and W. D. Gwinn, Calculation of Matrix Elements for One‐Dimensional Quantum‐Mechanical Problems and the Application to Anharmonic Oscillators, J. Chem. Phys. 43 (1965), 1515.

DOI: 10.1063/1.1696963

Google Scholar

[12] L.-Y. Peng and A. F. Starace, Application of Coulomb wave function discrete variable representation to atomic systems in strong laser fields, J. Chem. Phys.  125, (2006), 154311.

DOI: 10.1063/1.2358351

Google Scholar

[13] K. M. Dunseath, J. M. Launay, M. T. Dunseath and L. Mouret, Schwartz interpolation for problems involving the Coulomb potential, J. Phys. B 35 (2002), 3539.

DOI: 10.1088/0953-4075/35/16/313

Google Scholar

[14] C. Schwartz, High‐accuracy approximation techniques for analytic functions, J. Math. Phys. 26 (1985), 411.

Google Scholar

[15] A. K. Roy and S. I Chu, Density-functional calculations on singly and doubly excited Rydberg states of many-electron atoms, Phys. Rev. A 65 (2002), 052508.

DOI: 10.1103/physreva.65.052508

Google Scholar

[16] Ts. Tsednee and D. L. Yeager, A numerical Hartree self-consistent field calculation of an autoionization resonance parameters for a doubly excited 2s2, 3s2, and 4s2 states of He atom with a complex absorbing potential, Chin. Phys. B 26 (2017), 083101.

DOI: 10.1088/1674-1056/26/8/083101

Google Scholar

[17] Darío M. Mitnik, Helium atom in a box: Doubly excited levels within the 𝑆-wave model, Phys. Rev. A 70, 022703.

Google Scholar