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Correlation Energies of the Lithium Sequence

C. D. H. Chisholm

A. Dalgarno*

F. R. Innes

  • Department of Chemistry, Glasgow University, Glasgow, Scotland

  • School of Physics and Applied Mathematics, The Queen's University of Belfast, Belfast, Ireland

  • Air Force Cambridge Research Laboratories, Bedford, Massachusetts

  • *Present address: Smithsonian Astrophysical Observatory and Harvard College Observatory, Cambridge, Mass.

Phys. Rev. 167, 60 – Published 5 March, 1968

DOI: https://doi.org/10.1103/PhysRev.167.60

Abstract

The nonrelativistic eigenvalues of the 1s22pP2 states of the lithium sequence are calculated to be E(Z)=1.125Z2+1.09352614Z0.52717136+O(Z1) a.u., where Z is the nuclear charge; and the energy of the 1s22pP21s22sS2 transition is calculated to be ΔE(Z)=0.07072093Z0.11902237+O(Z1) a.u. For large nuclear charges, the addition of a 2p electron to the 1s2S1 core increases the magnitude of the correlation energy by 0.30 eV to give a value of 1.57 eV, most of which arises from the electron-pair energies.

References (6)

  1. C. D. H. Chisholm and A. Dalgarno, Proc. Roy. Soc. (London) A292, 264 (1966)
  2. M. Cohen, Proc. Phys. Soc. (London) 82, 778 (1963)
  3. C. W. Scherr, F. C. Sanders, and R. E. Knight, in Perturbation Theory and Its Applications in Quantum Mechanics, edited by C. H. Wilcox (John Wiley & Sons, Inc., New York, 1966), p. 97
  4. A. W. Weiss, Astrophys. J. 138, 1262 (1963)
  5. C. Froese, Astrophys. J. 141, 1206 (1965)
  6. A. Dalgarno, Proc. Phys. Soc. (London) 75, 439 (1960)

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