Electric Dipole Polarizability of Atoms by the Hartree—Fock Method. I. Theory for Closed-Shell Systems

  • Howard D. Cohen
    Laboratory of Molecular Structure and Spectra, Department of Physics, University of Chicago, Chicago, Illinois
  • C. C. J. Roothaan
    Laboratory of Molecular Structure and Spectra, Department of Physics, University of Chicago, Chicago, Illinois

書誌事項

公開日
1965-11-15
DOI
  • 10.1063/1.1701512
公開者
AIP Publishing

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説明

<jats:p>A method for the calculation of the dipole polarizabilities of closed-shell atomic systems is presented. This method involves the direct calculation of the Hartree—Fock wavefunction of the atom in the presence of the perturbing field. The orbitals are expressed as linear combinations of Slater-type functions. A large number of carefully chosen and optimized basis functions are used so as to assure a good fit to the true Hartree—Fock wavefunction. The polarizability is then calculated from the limiting value of α=p/F for F=0, where F is the electric field strength, and p is the induced dipole moment.</jats:p>

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