Abstract

A parametric model for lanthanide and actinide atomic and crystal energy levels is presented that correlates trends in Hartree–Fock calculations with empirically determined atomic parameters in such a way that predictions for unclassified complex cases can be made from the analysis of simpler ones. When appropriate effective operators, including electrostatic operators up to the third rank for fN configurations and magnetic operators up to the second rank for fN and fNd shells, are used in the parametric Hamiltonian, statistical errors of 10–20 cm−1 are typical for the simpler examples presented.

© 1984 Optical Society of America

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  1. E. U. Condon and G. H. Shortley, The Theory of Atomic Spectra (Cambridge U. Press, Cambridge, 1935, 1951).
  2. G. Racah, “Theory of complex spectra. II,” Phys. Rev. 62, 438–462 (1942); “Theory of complex spectra. III,”  63, 367–382 (1943); “Theory of complex spectra. IV,”  76, 1352–1365 (1949).
    [Crossref]
  3. U. Fano and G. Racah, Irreducible Tensorial Sets (Academic, New York, 1959).
  4. B. R. Judd, Operator Techniques in Atomic Spectroscopy (McGraw-Hill, New York, 1963).
  5. B. G. Wybourne, Spectroscopic Properties of Rare Earths (Interscience, New York, 1965).
  6. Z. B. Goldschmidt, “Atomic properties (free atom),” in Handbook on the Physics and Chemistry of Rare Earths, K. A. Gschneidner and L. Eyring, eds. (North-Holland, Amsterdam, 1978), Vol. I, Chap. I, pp. 1–247.
    [Crossref]
  7. R. D. Cowan, The Theory of Atomic Structure and Spectra (U. California Press, Berkeley, Calif., 1981).
  8. See, for instance, C. F. Fischer, The Hartree-Fock Method for Atoms (Wiley, New York, 1977).
  9. G. H. Dieke, Spectra and Energy Levels of Rare Earths Ions in Crystals (Interscience, New York, 1966).
  10. H. M. Crosswhite, “Systematic atomic and crystal-field parameters for lanthanides in LaCl3and LaF3,” in Spectroscopie des Éléments de Transition et des Éléments Lourdes dan Les Solides (Editions du CNRS, Paris, 1977), pp. 65–69.
  11. S. Hüfner, Optical Spectra of Transparent Rare Earth Compounds (Academic, New York, 1978).
  12. The program that we are using was adapted for us by M. Wilson from C. Froese-Fischer’s general multiconfiguration code [C. Froese-Fischer, “A multi-configuration Hartree-Fock program,” Comput. Phys. Commun. 1, 151–166 (1969)].
    [Crossref]
  13. R. D. Cowan and D. C. Griffin, “Approximate relativistic corrections to atomic radial wave functions,” J. Opt. Soc. Am. 66, 1010–1014 (1976).
    [Crossref]
  14. P. F. A. Klinkenberg and R. Lang, “The spectrum of trebly ionized thorium, Th iv,” Physica 15, 774–788 (1949).
    [Crossref]
  15. P. F. A. Klinkenberg, “Analysis of double ionized thorium, Th iii,” Physica 16, 618–650 (1950); G. Racah, “On the spectrum of Th iii,” Physica 16, 651–666 (1950).
    [Crossref]
  16. J. Sugar, “Analysis of the third spectrum of praseodymium,” J. Opt. Soc. Am. 53, 831–839 (1963); J. Res. Nat. Bur. Stand. (US) 73A, 333–351 (1969).
    [Crossref]
  17. C. E. Moore, Atomic Energy Levels as Derived from the Analysis of Atomic Spectra, U.S. Natl. Bur. Stand. Circ. 467, Vol.  III (1958); reissued as NSRDS-NBS 35 (U.S. Government Printing Office, Washington, D.C., 1971).
  18. V. Kaufman and L. J. Radziemski, “The sixth spectrum of uranium (U vi),” J. Opt. Soc. Am. 66, 599–600 (1976).
    [Crossref]
  19. W. C. Martin, R. Zalubas, and L. Hagan, Atomic Energy Levels—The Rare-Earth Elements, NSRDS-NBS 60 (U.S. Government Printing Office, Washington, D.C., 1978).
  20. J.-F. Wyart, V. Kaufman, and J. Sugar, “Analysis of the spectrum of four times-ionized uranium (U v),” Phys. Scr. 22, 389–396 (1980).
    [Crossref]
  21. C. H. H. Van Deurzen, K. Rajnak, and J. G. Conway, “Uranium five (U v), the 1S0level and a paramagnetic analysis of the 5f2 configuration,” J. Opt. Soc. Am. B 1, 45–47 (1984).
    [Crossref]
  22. H. H. Marvin, “Mutual magnetic interactions of electrons,” Phys. Rev. 71, 102–110 (1947).
    [Crossref]
  23. The Fischer program that we are using includes the Blume, Freeman, and Watson corrections to the spin–orbit integrals; see M. Blume and R. E. Watson, “Theory of spin–orbit coupling in atoms I. Derivation of the spin–orbit coupling constant,” Proc. R. Soc. Lond. Ser. A 270, 127–143 (1962); “II. Comparison of theory with experiment,” Proc. R. Soc. London Ser. 271, 565–578 (1963); M. Blume, A. J. Freeman, and R. E. Watson, “III.,” Phys. Rev. 134, A320–A327 (1964).
    [Crossref]
  24. These results are similar to those produced by R. D. Cowan’s HFR program. See Chap. 8 of his book.7
  25. R. E. Trees, “Configuration interaction in Mn ii,” Phys. Rev. 83, 756–760 (1951); “Term values in the 3d54s configuration of Fe iii,” Phys. Rev. 84, 1089–1091 (1951).
    [Crossref]
  26. K. Rajnak and B. G. Wybourne, “Configuration interaction effects in lN configurations,” Phys. Rev. 132, 280–290 (1963).
    [Crossref]
  27. B. R. Judd, J. E. Hansen, and A. J. J. Raassen, “Parametric fits in the atomic d shell,” J. Phys. B 15, 1457–1472 (1982).
    [Crossref]
  28. B. R. Judd and H. Crosswhite, “Orthogonalized operators for the f shell,” J. Opt. Soc. Am. B 1, 255–260 (1984).
    [Crossref]
  29. B. R. Judd, H. M. Crosswhite, and H. Crosswhite, “Inter-atomic magnetic interactions for f electrons,” Phys. Rev. 169, 130–138 (1968).
    [Crossref]
  30. Z. B. Goldschmidt, A. Pasternak, and Z. H. Goldschmidt, “Magnetic interactions in heavy atoms,” Phys. Lett. A 28, 265–266. (1968).
    [Crossref]
  31. B. R. Judd, “Three-particle operators for equivalent electrons,” Phys. Rev. 141, 4–14 (1966).
    [Crossref]
  32. J. C. Morrison, “Effect of core polarization upon the f–f interactions of rare-earth and actinide ions,” Phys. Rev. A 6, 643–650 (1972).
    [Crossref]
  33. D. J. Newman and C. D. Taylor, “Configuration interaction in rare-earth ions. I. Three-particle correlation in Pr2+,” J. Phys. B 4, 241–247 (1971).
    [Crossref]
  34. G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. II. Magnetic interactions,” J. Phys. B 4, 1388–1392 (1971).
    [Crossref]
  35. G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. III. Trees parameters for Pr2+ and Pr3+,” J. Phys. B 4, 1605–1610 (1971).
    [Crossref]
  36. H. Casimir, Proc. K. Ned. Akad. Wet. 34, 844 (1931).
  37. R. E. Trees, “The 4f3 and 4f25d configurations of doubly ionized praseodymium (Pr iii),” J. Opt. Soc. Am. 54, 651–657 (1964).
    [Crossref]
  38. Z. B. Goldschmidt, “Spin-dependent interactions in U v 5f2,” Phys. Rev. A 27, 740–753 (1983).
    [Crossref]
  39. N. Spector, “Configurations 4f36s and 4f36p in doubly ionized Pr,” J. Opt. Soc. Am. 54, 1359–1362 (1964).
    [Crossref]
  40. K. Rajnak, “Configuration interaction in the 4f3 configuration of Pr iii,” J. Opt. Soc. Am. 55, 126–132 (1965).
    [Crossref]
  41. H. Crosswhite, H. M. Crosswhite, and B. R. Judd, “Magnetic parameters for the configuration f3,” Phys. Rev. 174, 89–94 (1968).
    [Crossref]
  42. B. R. Judd, “Developments in atomic shell theory,” in The Structure of Matter, B. G. Wybourne, ed. (U. Canterbury Press, Christchurch, New Zealand, 1972); B. R. Judd and M. A. Suskin, “Complete set of orthogonal scalar operators for the configuration f3,” J. Opt. Soc. Am. B 1, 261–265 (1984).
    [Crossref]
  43. C. E. Schäffer and C. K. Jøgensen, “The nephelauxetic series of ligands corresponding to increasing tendency of partly covalent bonding,” J. Inorg. Nucl. Chem. 8, 143–148 (1958).
    [Crossref]
  44. H. Bethe, “Termaufspaltung in Kristallen Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 3, 133–208 (1929); Z. Phys. 60, 218 (1930) [English translation, Splitting of Terms of Crystals (Consultants Bureau, New York, undated).
    [Crossref]
  45. K. H. Hellwege, “Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 4, 95–160 (1949).
  46. A. Abragam and B. Bleaney, Electron Paramagnetic Resonance of Transition Ions (Clarendon, Oxford, 1970).
  47. H. M. Crosswhite and H. Crosswhite, “The spectrum of Nd3+:LaCl3,” J. Chem. Phys. 64, 1981–1985 (1976).
    [Crossref]
  48. W. T. Carnall, H. Crosswhite, H. M. Crosswhite, and J. G. Conway, “Energy level analysis of Pm3+:LaCl3,” J. Chem. Phys. 64, 3582–3591 (1976).
    [Crossref]
  49. M. S. Magno and G. H. Dieke, “Absorption and fluorescence spectra of hexagonal SmCl3and their Zeeman effects,” J. Chem. Phys. 37, 2354–2363 (1962); K. Rajnak, R. Mehlhorn, and N. Edelstein, “Calculation of the crystal field splitting of Sm3+levels in LaCl3with inclusion of J-mixing,” J. Chem. Phys. 58, 609–615 (1973); see also Ref. 9.
    [Crossref]
  50. H. M. Crosswhite and G. H. Dieke, “Spectrum and magnetic properties of hexagonal DyCl3,” J. Chem. Phys. 35, 1535–1548 (1961); see also Ref. 9.
    [Crossref]
  51. H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and K. Rajnak, “Parametric energy level analysis of Ho3+:LaCl3,” J. Chem. Phys. 67, 3002–3010 (1977).
    [Crossref]
  52. G. H. Dieke and S. Singh, “Absorption and fluorescence spectra with magnetic properties of ErCl3,” J. Chem. Phys. 35, 555–563 (1961); F. Varsanyi and G. H. Dieke, “Energy levels of hexagonal ErCl3,” J. Chem. Phys. 36, 2951–2961 (1962); see also Ref. 9.
    [Crossref]
  53. H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and A. P. Paszek, “Spectrum analysis of U3+:LaCl3,” J. Chem. Phys. 72, 5103–5117 (1980).
    [Crossref]
  54. W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
    [Crossref]
  55. H. Lammerman and J. G. Conway, “Absorption spectrum of Pu3+in lanthanum trichloride and lanthanum ethylsulfate,” J. Chem. Phys. 38, 259–269 (1963); J. G. Conway and K. Rajnak, J. Chem. Phys. 44, 348–354 (1966).
    [Crossref]
  56. J. Blaise, Laboratoire Aimé Cotton, Orsay, France; J. G. Conway and E. Worden, Lawrence Livermore National Laboratory, Berkeley, California 94720 (personal communication).
  57. S. Feneuille and N. Pelletier-Allard, “Contribution a l’interpretation des configurations 4f26s, 4f25d et 4f26pde Pr iii,” Phys. (Utrecht) 40, 347–356 (1968).
    [Crossref]
  58. J.-F. Wyart, J. Blaise, and P. Camus, “Progres récent dans l’interprétation des configurations 4fN(5d+ 6s) des lanthanides,” Phys. Scr. 9, 325–330 (1974).
    [Crossref]
  59. H. M. Crosswhite, “Effective electrostatic operators for two inequivalent electrons,” Phys. Rev. A 4, 485–489 (1971).
    [Crossref]
  60. J. Sugar and V. Kaufman, “Spectra and energy levels of three-and four-times ionized hafnium (Hf iv and HF v),” J. Opt. Soc. Am. 64, 1656–1664 (1974).
    [Crossref]
  61. V. Kaufman and J. Sugar, “Spectra and energy levels of five-times ionized tantalum (Ta vi),” J. Opt. Soc. Am. 65, 302–309 (1975).
    [Crossref]
  62. J. Sugar and V. Kaufman, “Seventh spectrum of tungsten (W vii); resonance lines of Hf v,” Phys. Rev. A 12, 994–1012 (1975).
    [Crossref]
  63. J. G. Conway, J. Blaise, and Jean Vergés, “The I.R. spectrum of curium-244,” Spectrochim. Acta Part B,  31, 31–47 (1976).
    [Crossref]

1984 (2)

1983 (1)

Z. B. Goldschmidt, “Spin-dependent interactions in U v 5f2,” Phys. Rev. A 27, 740–753 (1983).
[Crossref]

1982 (1)

B. R. Judd, J. E. Hansen, and A. J. J. Raassen, “Parametric fits in the atomic d shell,” J. Phys. B 15, 1457–1472 (1982).
[Crossref]

1980 (3)

J.-F. Wyart, V. Kaufman, and J. Sugar, “Analysis of the spectrum of four times-ionized uranium (U v),” Phys. Scr. 22, 389–396 (1980).
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and A. P. Paszek, “Spectrum analysis of U3+:LaCl3,” J. Chem. Phys. 72, 5103–5117 (1980).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

1977 (1)

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and K. Rajnak, “Parametric energy level analysis of Ho3+:LaCl3,” J. Chem. Phys. 67, 3002–3010 (1977).
[Crossref]

1976 (5)

J. G. Conway, J. Blaise, and Jean Vergés, “The I.R. spectrum of curium-244,” Spectrochim. Acta Part B,  31, 31–47 (1976).
[Crossref]

H. M. Crosswhite and H. Crosswhite, “The spectrum of Nd3+:LaCl3,” J. Chem. Phys. 64, 1981–1985 (1976).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, and J. G. Conway, “Energy level analysis of Pm3+:LaCl3,” J. Chem. Phys. 64, 3582–3591 (1976).
[Crossref]

R. D. Cowan and D. C. Griffin, “Approximate relativistic corrections to atomic radial wave functions,” J. Opt. Soc. Am. 66, 1010–1014 (1976).
[Crossref]

V. Kaufman and L. J. Radziemski, “The sixth spectrum of uranium (U vi),” J. Opt. Soc. Am. 66, 599–600 (1976).
[Crossref]

1975 (2)

V. Kaufman and J. Sugar, “Spectra and energy levels of five-times ionized tantalum (Ta vi),” J. Opt. Soc. Am. 65, 302–309 (1975).
[Crossref]

J. Sugar and V. Kaufman, “Seventh spectrum of tungsten (W vii); resonance lines of Hf v,” Phys. Rev. A 12, 994–1012 (1975).
[Crossref]

1974 (2)

J. Sugar and V. Kaufman, “Spectra and energy levels of three-and four-times ionized hafnium (Hf iv and HF v),” J. Opt. Soc. Am. 64, 1656–1664 (1974).
[Crossref]

J.-F. Wyart, J. Blaise, and P. Camus, “Progres récent dans l’interprétation des configurations 4fN(5d+ 6s) des lanthanides,” Phys. Scr. 9, 325–330 (1974).
[Crossref]

1972 (1)

J. C. Morrison, “Effect of core polarization upon the f–f interactions of rare-earth and actinide ions,” Phys. Rev. A 6, 643–650 (1972).
[Crossref]

1971 (4)

D. J. Newman and C. D. Taylor, “Configuration interaction in rare-earth ions. I. Three-particle correlation in Pr2+,” J. Phys. B 4, 241–247 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. II. Magnetic interactions,” J. Phys. B 4, 1388–1392 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. III. Trees parameters for Pr2+ and Pr3+,” J. Phys. B 4, 1605–1610 (1971).
[Crossref]

H. M. Crosswhite, “Effective electrostatic operators for two inequivalent electrons,” Phys. Rev. A 4, 485–489 (1971).
[Crossref]

1969 (1)

The program that we are using was adapted for us by M. Wilson from C. Froese-Fischer’s general multiconfiguration code [C. Froese-Fischer, “A multi-configuration Hartree-Fock program,” Comput. Phys. Commun. 1, 151–166 (1969)].
[Crossref]

1968 (4)

B. R. Judd, H. M. Crosswhite, and H. Crosswhite, “Inter-atomic magnetic interactions for f electrons,” Phys. Rev. 169, 130–138 (1968).
[Crossref]

Z. B. Goldschmidt, A. Pasternak, and Z. H. Goldschmidt, “Magnetic interactions in heavy atoms,” Phys. Lett. A 28, 265–266. (1968).
[Crossref]

H. Crosswhite, H. M. Crosswhite, and B. R. Judd, “Magnetic parameters for the configuration f3,” Phys. Rev. 174, 89–94 (1968).
[Crossref]

S. Feneuille and N. Pelletier-Allard, “Contribution a l’interpretation des configurations 4f26s, 4f25d et 4f26pde Pr iii,” Phys. (Utrecht) 40, 347–356 (1968).
[Crossref]

1966 (1)

B. R. Judd, “Three-particle operators for equivalent electrons,” Phys. Rev. 141, 4–14 (1966).
[Crossref]

1965 (1)

1964 (2)

1963 (3)

K. Rajnak and B. G. Wybourne, “Configuration interaction effects in lN configurations,” Phys. Rev. 132, 280–290 (1963).
[Crossref]

J. Sugar, “Analysis of the third spectrum of praseodymium,” J. Opt. Soc. Am. 53, 831–839 (1963); J. Res. Nat. Bur. Stand. (US) 73A, 333–351 (1969).
[Crossref]

H. Lammerman and J. G. Conway, “Absorption spectrum of Pu3+in lanthanum trichloride and lanthanum ethylsulfate,” J. Chem. Phys. 38, 259–269 (1963); J. G. Conway and K. Rajnak, J. Chem. Phys. 44, 348–354 (1966).
[Crossref]

1962 (2)

The Fischer program that we are using includes the Blume, Freeman, and Watson corrections to the spin–orbit integrals; see M. Blume and R. E. Watson, “Theory of spin–orbit coupling in atoms I. Derivation of the spin–orbit coupling constant,” Proc. R. Soc. Lond. Ser. A 270, 127–143 (1962); “II. Comparison of theory with experiment,” Proc. R. Soc. London Ser. 271, 565–578 (1963); M. Blume, A. J. Freeman, and R. E. Watson, “III.,” Phys. Rev. 134, A320–A327 (1964).
[Crossref]

M. S. Magno and G. H. Dieke, “Absorption and fluorescence spectra of hexagonal SmCl3and their Zeeman effects,” J. Chem. Phys. 37, 2354–2363 (1962); K. Rajnak, R. Mehlhorn, and N. Edelstein, “Calculation of the crystal field splitting of Sm3+levels in LaCl3with inclusion of J-mixing,” J. Chem. Phys. 58, 609–615 (1973); see also Ref. 9.
[Crossref]

1961 (2)

H. M. Crosswhite and G. H. Dieke, “Spectrum and magnetic properties of hexagonal DyCl3,” J. Chem. Phys. 35, 1535–1548 (1961); see also Ref. 9.
[Crossref]

G. H. Dieke and S. Singh, “Absorption and fluorescence spectra with magnetic properties of ErCl3,” J. Chem. Phys. 35, 555–563 (1961); F. Varsanyi and G. H. Dieke, “Energy levels of hexagonal ErCl3,” J. Chem. Phys. 36, 2951–2961 (1962); see also Ref. 9.
[Crossref]

1958 (2)

C. E. Schäffer and C. K. Jøgensen, “The nephelauxetic series of ligands corresponding to increasing tendency of partly covalent bonding,” J. Inorg. Nucl. Chem. 8, 143–148 (1958).
[Crossref]

C. E. Moore, Atomic Energy Levels as Derived from the Analysis of Atomic Spectra, U.S. Natl. Bur. Stand. Circ. 467, Vol.  III (1958); reissued as NSRDS-NBS 35 (U.S. Government Printing Office, Washington, D.C., 1971).

1951 (1)

R. E. Trees, “Configuration interaction in Mn ii,” Phys. Rev. 83, 756–760 (1951); “Term values in the 3d54s configuration of Fe iii,” Phys. Rev. 84, 1089–1091 (1951).
[Crossref]

1950 (1)

P. F. A. Klinkenberg, “Analysis of double ionized thorium, Th iii,” Physica 16, 618–650 (1950); G. Racah, “On the spectrum of Th iii,” Physica 16, 651–666 (1950).
[Crossref]

1949 (2)

P. F. A. Klinkenberg and R. Lang, “The spectrum of trebly ionized thorium, Th iv,” Physica 15, 774–788 (1949).
[Crossref]

K. H. Hellwege, “Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 4, 95–160 (1949).

1947 (1)

H. H. Marvin, “Mutual magnetic interactions of electrons,” Phys. Rev. 71, 102–110 (1947).
[Crossref]

1942 (1)

G. Racah, “Theory of complex spectra. II,” Phys. Rev. 62, 438–462 (1942); “Theory of complex spectra. III,”  63, 367–382 (1943); “Theory of complex spectra. IV,”  76, 1352–1365 (1949).
[Crossref]

1931 (1)

H. Casimir, Proc. K. Ned. Akad. Wet. 34, 844 (1931).

1929 (1)

H. Bethe, “Termaufspaltung in Kristallen Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 3, 133–208 (1929); Z. Phys. 60, 218 (1930) [English translation, Splitting of Terms of Crystals (Consultants Bureau, New York, undated).
[Crossref]

Abragam, A.

A. Abragam and B. Bleaney, Electron Paramagnetic Resonance of Transition Ions (Clarendon, Oxford, 1970).

Bethe, H.

H. Bethe, “Termaufspaltung in Kristallen Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 3, 133–208 (1929); Z. Phys. 60, 218 (1930) [English translation, Splitting of Terms of Crystals (Consultants Bureau, New York, undated).
[Crossref]

Blaise, J.

J. G. Conway, J. Blaise, and Jean Vergés, “The I.R. spectrum of curium-244,” Spectrochim. Acta Part B,  31, 31–47 (1976).
[Crossref]

J.-F. Wyart, J. Blaise, and P. Camus, “Progres récent dans l’interprétation des configurations 4fN(5d+ 6s) des lanthanides,” Phys. Scr. 9, 325–330 (1974).
[Crossref]

J. Blaise, Laboratoire Aimé Cotton, Orsay, France; J. G. Conway and E. Worden, Lawrence Livermore National Laboratory, Berkeley, California 94720 (personal communication).

Bleaney, B.

A. Abragam and B. Bleaney, Electron Paramagnetic Resonance of Transition Ions (Clarendon, Oxford, 1970).

Blume, M.

The Fischer program that we are using includes the Blume, Freeman, and Watson corrections to the spin–orbit integrals; see M. Blume and R. E. Watson, “Theory of spin–orbit coupling in atoms I. Derivation of the spin–orbit coupling constant,” Proc. R. Soc. Lond. Ser. A 270, 127–143 (1962); “II. Comparison of theory with experiment,” Proc. R. Soc. London Ser. 271, 565–578 (1963); M. Blume, A. J. Freeman, and R. E. Watson, “III.,” Phys. Rev. 134, A320–A327 (1964).
[Crossref]

Camus, P.

J.-F. Wyart, J. Blaise, and P. Camus, “Progres récent dans l’interprétation des configurations 4fN(5d+ 6s) des lanthanides,” Phys. Scr. 9, 325–330 (1974).
[Crossref]

Carnall, W. T.

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and A. P. Paszek, “Spectrum analysis of U3+:LaCl3,” J. Chem. Phys. 72, 5103–5117 (1980).
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and K. Rajnak, “Parametric energy level analysis of Ho3+:LaCl3,” J. Chem. Phys. 67, 3002–3010 (1977).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, and J. G. Conway, “Energy level analysis of Pm3+:LaCl3,” J. Chem. Phys. 64, 3582–3591 (1976).
[Crossref]

Casimir, H.

H. Casimir, Proc. K. Ned. Akad. Wet. 34, 844 (1931).

Condon, E. U.

E. U. Condon and G. H. Shortley, The Theory of Atomic Spectra (Cambridge U. Press, Cambridge, 1935, 1951).

Conway, J. G.

C. H. H. Van Deurzen, K. Rajnak, and J. G. Conway, “Uranium five (U v), the 1S0level and a paramagnetic analysis of the 5f2 configuration,” J. Opt. Soc. Am. B 1, 45–47 (1984).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, and J. G. Conway, “Energy level analysis of Pm3+:LaCl3,” J. Chem. Phys. 64, 3582–3591 (1976).
[Crossref]

J. G. Conway, J. Blaise, and Jean Vergés, “The I.R. spectrum of curium-244,” Spectrochim. Acta Part B,  31, 31–47 (1976).
[Crossref]

H. Lammerman and J. G. Conway, “Absorption spectrum of Pu3+in lanthanum trichloride and lanthanum ethylsulfate,” J. Chem. Phys. 38, 259–269 (1963); J. G. Conway and K. Rajnak, J. Chem. Phys. 44, 348–354 (1966).
[Crossref]

Copland, G. M.

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. III. Trees parameters for Pr2+ and Pr3+,” J. Phys. B 4, 1605–1610 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. II. Magnetic interactions,” J. Phys. B 4, 1388–1392 (1971).
[Crossref]

Cowan, R. D.

Crosswhite, H.

B. R. Judd and H. Crosswhite, “Orthogonalized operators for the f shell,” J. Opt. Soc. Am. B 1, 255–260 (1984).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and A. P. Paszek, “Spectrum analysis of U3+:LaCl3,” J. Chem. Phys. 72, 5103–5117 (1980).
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and K. Rajnak, “Parametric energy level analysis of Ho3+:LaCl3,” J. Chem. Phys. 67, 3002–3010 (1977).
[Crossref]

H. M. Crosswhite and H. Crosswhite, “The spectrum of Nd3+:LaCl3,” J. Chem. Phys. 64, 1981–1985 (1976).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, and J. G. Conway, “Energy level analysis of Pm3+:LaCl3,” J. Chem. Phys. 64, 3582–3591 (1976).
[Crossref]

B. R. Judd, H. M. Crosswhite, and H. Crosswhite, “Inter-atomic magnetic interactions for f electrons,” Phys. Rev. 169, 130–138 (1968).
[Crossref]

H. Crosswhite, H. M. Crosswhite, and B. R. Judd, “Magnetic parameters for the configuration f3,” Phys. Rev. 174, 89–94 (1968).
[Crossref]

Crosswhite, H. M.

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and A. P. Paszek, “Spectrum analysis of U3+:LaCl3,” J. Chem. Phys. 72, 5103–5117 (1980).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and K. Rajnak, “Parametric energy level analysis of Ho3+:LaCl3,” J. Chem. Phys. 67, 3002–3010 (1977).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, and J. G. Conway, “Energy level analysis of Pm3+:LaCl3,” J. Chem. Phys. 64, 3582–3591 (1976).
[Crossref]

H. M. Crosswhite and H. Crosswhite, “The spectrum of Nd3+:LaCl3,” J. Chem. Phys. 64, 1981–1985 (1976).
[Crossref]

H. M. Crosswhite, “Effective electrostatic operators for two inequivalent electrons,” Phys. Rev. A 4, 485–489 (1971).
[Crossref]

H. Crosswhite, H. M. Crosswhite, and B. R. Judd, “Magnetic parameters for the configuration f3,” Phys. Rev. 174, 89–94 (1968).
[Crossref]

B. R. Judd, H. M. Crosswhite, and H. Crosswhite, “Inter-atomic magnetic interactions for f electrons,” Phys. Rev. 169, 130–138 (1968).
[Crossref]

H. M. Crosswhite and G. H. Dieke, “Spectrum and magnetic properties of hexagonal DyCl3,” J. Chem. Phys. 35, 1535–1548 (1961); see also Ref. 9.
[Crossref]

H. M. Crosswhite, “Systematic atomic and crystal-field parameters for lanthanides in LaCl3and LaF3,” in Spectroscopie des Éléments de Transition et des Éléments Lourdes dan Les Solides (Editions du CNRS, Paris, 1977), pp. 65–69.

Dieke, G. H.

M. S. Magno and G. H. Dieke, “Absorption and fluorescence spectra of hexagonal SmCl3and their Zeeman effects,” J. Chem. Phys. 37, 2354–2363 (1962); K. Rajnak, R. Mehlhorn, and N. Edelstein, “Calculation of the crystal field splitting of Sm3+levels in LaCl3with inclusion of J-mixing,” J. Chem. Phys. 58, 609–615 (1973); see also Ref. 9.
[Crossref]

H. M. Crosswhite and G. H. Dieke, “Spectrum and magnetic properties of hexagonal DyCl3,” J. Chem. Phys. 35, 1535–1548 (1961); see also Ref. 9.
[Crossref]

G. H. Dieke and S. Singh, “Absorption and fluorescence spectra with magnetic properties of ErCl3,” J. Chem. Phys. 35, 555–563 (1961); F. Varsanyi and G. H. Dieke, “Energy levels of hexagonal ErCl3,” J. Chem. Phys. 36, 2951–2961 (1962); see also Ref. 9.
[Crossref]

G. H. Dieke, Spectra and Energy Levels of Rare Earths Ions in Crystals (Interscience, New York, 1966).

Edelstein, N.

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

Fano, U.

U. Fano and G. Racah, Irreducible Tensorial Sets (Academic, New York, 1959).

Feneuille, S.

S. Feneuille and N. Pelletier-Allard, “Contribution a l’interpretation des configurations 4f26s, 4f25d et 4f26pde Pr iii,” Phys. (Utrecht) 40, 347–356 (1968).
[Crossref]

Fischer, C. F.

See, for instance, C. F. Fischer, The Hartree-Fock Method for Atoms (Wiley, New York, 1977).

Froese-Fischer, C.

The program that we are using was adapted for us by M. Wilson from C. Froese-Fischer’s general multiconfiguration code [C. Froese-Fischer, “A multi-configuration Hartree-Fock program,” Comput. Phys. Commun. 1, 151–166 (1969)].
[Crossref]

Goldschmidt, Z. B.

Z. B. Goldschmidt, “Spin-dependent interactions in U v 5f2,” Phys. Rev. A 27, 740–753 (1983).
[Crossref]

Z. B. Goldschmidt, A. Pasternak, and Z. H. Goldschmidt, “Magnetic interactions in heavy atoms,” Phys. Lett. A 28, 265–266. (1968).
[Crossref]

Z. B. Goldschmidt, “Atomic properties (free atom),” in Handbook on the Physics and Chemistry of Rare Earths, K. A. Gschneidner and L. Eyring, eds. (North-Holland, Amsterdam, 1978), Vol. I, Chap. I, pp. 1–247.
[Crossref]

Goldschmidt, Z. H.

Z. B. Goldschmidt, A. Pasternak, and Z. H. Goldschmidt, “Magnetic interactions in heavy atoms,” Phys. Lett. A 28, 265–266. (1968).
[Crossref]

Griffin, D. C.

Hagan, L.

W. C. Martin, R. Zalubas, and L. Hagan, Atomic Energy Levels—The Rare-Earth Elements, NSRDS-NBS 60 (U.S. Government Printing Office, Washington, D.C., 1978).

Hansen, J. E.

B. R. Judd, J. E. Hansen, and A. J. J. Raassen, “Parametric fits in the atomic d shell,” J. Phys. B 15, 1457–1472 (1982).
[Crossref]

Hellwege, K. H.

K. H. Hellwege, “Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 4, 95–160 (1949).

Hessler, J. P.

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

Hüfner, S.

S. Hüfner, Optical Spectra of Transparent Rare Earth Compounds (Academic, New York, 1978).

Jøgensen, C. K.

C. E. Schäffer and C. K. Jøgensen, “The nephelauxetic series of ligands corresponding to increasing tendency of partly covalent bonding,” J. Inorg. Nucl. Chem. 8, 143–148 (1958).
[Crossref]

Judd, B. R.

B. R. Judd and H. Crosswhite, “Orthogonalized operators for the f shell,” J. Opt. Soc. Am. B 1, 255–260 (1984).
[Crossref]

B. R. Judd, J. E. Hansen, and A. J. J. Raassen, “Parametric fits in the atomic d shell,” J. Phys. B 15, 1457–1472 (1982).
[Crossref]

B. R. Judd, H. M. Crosswhite, and H. Crosswhite, “Inter-atomic magnetic interactions for f electrons,” Phys. Rev. 169, 130–138 (1968).
[Crossref]

H. Crosswhite, H. M. Crosswhite, and B. R. Judd, “Magnetic parameters for the configuration f3,” Phys. Rev. 174, 89–94 (1968).
[Crossref]

B. R. Judd, “Three-particle operators for equivalent electrons,” Phys. Rev. 141, 4–14 (1966).
[Crossref]

B. R. Judd, “Developments in atomic shell theory,” in The Structure of Matter, B. G. Wybourne, ed. (U. Canterbury Press, Christchurch, New Zealand, 1972); B. R. Judd and M. A. Suskin, “Complete set of orthogonal scalar operators for the configuration f3,” J. Opt. Soc. Am. B 1, 261–265 (1984).
[Crossref]

B. R. Judd, Operator Techniques in Atomic Spectroscopy (McGraw-Hill, New York, 1963).

Kaufman, V.

Klinkenberg, P. F. A.

P. F. A. Klinkenberg, “Analysis of double ionized thorium, Th iii,” Physica 16, 618–650 (1950); G. Racah, “On the spectrum of Th iii,” Physica 16, 651–666 (1950).
[Crossref]

P. F. A. Klinkenberg and R. Lang, “The spectrum of trebly ionized thorium, Th iv,” Physica 15, 774–788 (1949).
[Crossref]

Lammerman, H.

H. Lammerman and J. G. Conway, “Absorption spectrum of Pu3+in lanthanum trichloride and lanthanum ethylsulfate,” J. Chem. Phys. 38, 259–269 (1963); J. G. Conway and K. Rajnak, J. Chem. Phys. 44, 348–354 (1966).
[Crossref]

Lang, R.

P. F. A. Klinkenberg and R. Lang, “The spectrum of trebly ionized thorium, Th iv,” Physica 15, 774–788 (1949).
[Crossref]

Magno, M. S.

M. S. Magno and G. H. Dieke, “Absorption and fluorescence spectra of hexagonal SmCl3and their Zeeman effects,” J. Chem. Phys. 37, 2354–2363 (1962); K. Rajnak, R. Mehlhorn, and N. Edelstein, “Calculation of the crystal field splitting of Sm3+levels in LaCl3with inclusion of J-mixing,” J. Chem. Phys. 58, 609–615 (1973); see also Ref. 9.
[Crossref]

Martin, W. C.

W. C. Martin, R. Zalubas, and L. Hagan, Atomic Energy Levels—The Rare-Earth Elements, NSRDS-NBS 60 (U.S. Government Printing Office, Washington, D.C., 1978).

Marvin, H. H.

H. H. Marvin, “Mutual magnetic interactions of electrons,” Phys. Rev. 71, 102–110 (1947).
[Crossref]

Moore, C. E.

C. E. Moore, Atomic Energy Levels as Derived from the Analysis of Atomic Spectra, U.S. Natl. Bur. Stand. Circ. 467, Vol.  III (1958); reissued as NSRDS-NBS 35 (U.S. Government Printing Office, Washington, D.C., 1971).

Morrison, J. C.

J. C. Morrison, “Effect of core polarization upon the f–f interactions of rare-earth and actinide ions,” Phys. Rev. A 6, 643–650 (1972).
[Crossref]

Newman, D. J.

D. J. Newman and C. D. Taylor, “Configuration interaction in rare-earth ions. I. Three-particle correlation in Pr2+,” J. Phys. B 4, 241–247 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. II. Magnetic interactions,” J. Phys. B 4, 1388–1392 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. III. Trees parameters for Pr2+ and Pr3+,” J. Phys. B 4, 1605–1610 (1971).
[Crossref]

Pasternak, A.

Z. B. Goldschmidt, A. Pasternak, and Z. H. Goldschmidt, “Magnetic interactions in heavy atoms,” Phys. Lett. A 28, 265–266. (1968).
[Crossref]

Paszek, A. P.

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and A. P. Paszek, “Spectrum analysis of U3+:LaCl3,” J. Chem. Phys. 72, 5103–5117 (1980).
[Crossref]

Pelletier-Allard, N.

S. Feneuille and N. Pelletier-Allard, “Contribution a l’interpretation des configurations 4f26s, 4f25d et 4f26pde Pr iii,” Phys. (Utrecht) 40, 347–356 (1968).
[Crossref]

Raassen, A. J. J.

B. R. Judd, J. E. Hansen, and A. J. J. Raassen, “Parametric fits in the atomic d shell,” J. Phys. B 15, 1457–1472 (1982).
[Crossref]

Racah, G.

G. Racah, “Theory of complex spectra. II,” Phys. Rev. 62, 438–462 (1942); “Theory of complex spectra. III,”  63, 367–382 (1943); “Theory of complex spectra. IV,”  76, 1352–1365 (1949).
[Crossref]

U. Fano and G. Racah, Irreducible Tensorial Sets (Academic, New York, 1959).

Radziemski, L. J.

Rajnak, K.

C. H. H. Van Deurzen, K. Rajnak, and J. G. Conway, “Uranium five (U v), the 1S0level and a paramagnetic analysis of the 5f2 configuration,” J. Opt. Soc. Am. B 1, 45–47 (1984).
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and K. Rajnak, “Parametric energy level analysis of Ho3+:LaCl3,” J. Chem. Phys. 67, 3002–3010 (1977).
[Crossref]

K. Rajnak, “Configuration interaction in the 4f3 configuration of Pr iii,” J. Opt. Soc. Am. 55, 126–132 (1965).
[Crossref]

K. Rajnak and B. G. Wybourne, “Configuration interaction effects in lN configurations,” Phys. Rev. 132, 280–290 (1963).
[Crossref]

Sarup, R.

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

Schäffer, C. E.

C. E. Schäffer and C. K. Jøgensen, “The nephelauxetic series of ligands corresponding to increasing tendency of partly covalent bonding,” J. Inorg. Nucl. Chem. 8, 143–148 (1958).
[Crossref]

Shalimoff, G. V.

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

Shortley, G. H.

E. U. Condon and G. H. Shortley, The Theory of Atomic Spectra (Cambridge U. Press, Cambridge, 1935, 1951).

Singh, S.

G. H. Dieke and S. Singh, “Absorption and fluorescence spectra with magnetic properties of ErCl3,” J. Chem. Phys. 35, 555–563 (1961); F. Varsanyi and G. H. Dieke, “Energy levels of hexagonal ErCl3,” J. Chem. Phys. 36, 2951–2961 (1962); see also Ref. 9.
[Crossref]

Spector, N.

Sugar, J.

Taylor, C. D.

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. II. Magnetic interactions,” J. Phys. B 4, 1388–1392 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. III. Trees parameters for Pr2+ and Pr3+,” J. Phys. B 4, 1605–1610 (1971).
[Crossref]

D. J. Newman and C. D. Taylor, “Configuration interaction in rare-earth ions. I. Three-particle correlation in Pr2+,” J. Phys. B 4, 241–247 (1971).
[Crossref]

Trees, R. E.

R. E. Trees, “The 4f3 and 4f25d configurations of doubly ionized praseodymium (Pr iii),” J. Opt. Soc. Am. 54, 651–657 (1964).
[Crossref]

R. E. Trees, “Configuration interaction in Mn ii,” Phys. Rev. 83, 756–760 (1951); “Term values in the 3d54s configuration of Fe iii,” Phys. Rev. 84, 1089–1091 (1951).
[Crossref]

Van Deurzen, C. H. H.

Vergés, Jean

J. G. Conway, J. Blaise, and Jean Vergés, “The I.R. spectrum of curium-244,” Spectrochim. Acta Part B,  31, 31–47 (1976).
[Crossref]

Watson, R. E.

The Fischer program that we are using includes the Blume, Freeman, and Watson corrections to the spin–orbit integrals; see M. Blume and R. E. Watson, “Theory of spin–orbit coupling in atoms I. Derivation of the spin–orbit coupling constant,” Proc. R. Soc. Lond. Ser. A 270, 127–143 (1962); “II. Comparison of theory with experiment,” Proc. R. Soc. London Ser. 271, 565–578 (1963); M. Blume, A. J. Freeman, and R. E. Watson, “III.,” Phys. Rev. 134, A320–A327 (1964).
[Crossref]

Wyart, J.-F.

J.-F. Wyart, V. Kaufman, and J. Sugar, “Analysis of the spectrum of four times-ionized uranium (U v),” Phys. Scr. 22, 389–396 (1980).
[Crossref]

J.-F. Wyart, J. Blaise, and P. Camus, “Progres récent dans l’interprétation des configurations 4fN(5d+ 6s) des lanthanides,” Phys. Scr. 9, 325–330 (1974).
[Crossref]

Wybourne, B. G.

K. Rajnak and B. G. Wybourne, “Configuration interaction effects in lN configurations,” Phys. Rev. 132, 280–290 (1963).
[Crossref]

B. G. Wybourne, Spectroscopic Properties of Rare Earths (Interscience, New York, 1965).

Zalubas, R.

W. C. Martin, R. Zalubas, and L. Hagan, Atomic Energy Levels—The Rare-Earth Elements, NSRDS-NBS 60 (U.S. Government Printing Office, Washington, D.C., 1978).

Ann. Phys. (2)

H. Bethe, “Termaufspaltung in Kristallen Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 3, 133–208 (1929); Z. Phys. 60, 218 (1930) [English translation, Splitting of Terms of Crystals (Consultants Bureau, New York, undated).
[Crossref]

K. H. Hellwege, “Electronenterme und Strahlung von Atomen in Kristallen,” Ann. Phys. 4, 95–160 (1949).

Atomic Energy Levels as Derived from the Analysis of Atomic Spectra (1)

C. E. Moore, Atomic Energy Levels as Derived from the Analysis of Atomic Spectra, U.S. Natl. Bur. Stand. Circ. 467, Vol.  III (1958); reissued as NSRDS-NBS 35 (U.S. Government Printing Office, Washington, D.C., 1971).

Comput. Phys. Commun. (1)

The program that we are using was adapted for us by M. Wilson from C. Froese-Fischer’s general multiconfiguration code [C. Froese-Fischer, “A multi-configuration Hartree-Fock program,” Comput. Phys. Commun. 1, 151–166 (1969)].
[Crossref]

J. Chem. Phys. (9)

H. M. Crosswhite and H. Crosswhite, “The spectrum of Nd3+:LaCl3,” J. Chem. Phys. 64, 1981–1985 (1976).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, and J. G. Conway, “Energy level analysis of Pm3+:LaCl3,” J. Chem. Phys. 64, 3582–3591 (1976).
[Crossref]

M. S. Magno and G. H. Dieke, “Absorption and fluorescence spectra of hexagonal SmCl3and their Zeeman effects,” J. Chem. Phys. 37, 2354–2363 (1962); K. Rajnak, R. Mehlhorn, and N. Edelstein, “Calculation of the crystal field splitting of Sm3+levels in LaCl3with inclusion of J-mixing,” J. Chem. Phys. 58, 609–615 (1973); see also Ref. 9.
[Crossref]

H. M. Crosswhite and G. H. Dieke, “Spectrum and magnetic properties of hexagonal DyCl3,” J. Chem. Phys. 35, 1535–1548 (1961); see also Ref. 9.
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and K. Rajnak, “Parametric energy level analysis of Ho3+:LaCl3,” J. Chem. Phys. 67, 3002–3010 (1977).
[Crossref]

G. H. Dieke and S. Singh, “Absorption and fluorescence spectra with magnetic properties of ErCl3,” J. Chem. Phys. 35, 555–563 (1961); F. Varsanyi and G. H. Dieke, “Energy levels of hexagonal ErCl3,” J. Chem. Phys. 36, 2951–2961 (1962); see also Ref. 9.
[Crossref]

H. M. Crosswhite, H. Crosswhite, W. T. Carnall, and A. P. Paszek, “Spectrum analysis of U3+:LaCl3,” J. Chem. Phys. 72, 5103–5117 (1980).
[Crossref]

W. T. Carnall, H. Crosswhite, H. M. Crosswhite, J. P. Hessler, N. Edelstein, J. G. Conway, G. V. Shalimoff, and R. Sarup, “Energy level analysis of Np3+:LaCl3and Np3+:LaBr3,” J. Chem. Phys. 72, 5089–5102 (1980).
[Crossref]

H. Lammerman and J. G. Conway, “Absorption spectrum of Pu3+in lanthanum trichloride and lanthanum ethylsulfate,” J. Chem. Phys. 38, 259–269 (1963); J. G. Conway and K. Rajnak, J. Chem. Phys. 44, 348–354 (1966).
[Crossref]

J. Inorg. Nucl. Chem. (1)

C. E. Schäffer and C. K. Jøgensen, “The nephelauxetic series of ligands corresponding to increasing tendency of partly covalent bonding,” J. Inorg. Nucl. Chem. 8, 143–148 (1958).
[Crossref]

J. Opt. Soc. Am. (8)

J. Opt. Soc. Am. B (2)

J. Phys. B (4)

D. J. Newman and C. D. Taylor, “Configuration interaction in rare-earth ions. I. Three-particle correlation in Pr2+,” J. Phys. B 4, 241–247 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. II. Magnetic interactions,” J. Phys. B 4, 1388–1392 (1971).
[Crossref]

G. M. Copland, D. J. Newman, and C. D. Taylor, “Configuration interaction in rare-earth ions. III. Trees parameters for Pr2+ and Pr3+,” J. Phys. B 4, 1605–1610 (1971).
[Crossref]

B. R. Judd, J. E. Hansen, and A. J. J. Raassen, “Parametric fits in the atomic d shell,” J. Phys. B 15, 1457–1472 (1982).
[Crossref]

Phys. (Utrecht) (1)

S. Feneuille and N. Pelletier-Allard, “Contribution a l’interpretation des configurations 4f26s, 4f25d et 4f26pde Pr iii,” Phys. (Utrecht) 40, 347–356 (1968).
[Crossref]

Phys. Lett. A (1)

Z. B. Goldschmidt, A. Pasternak, and Z. H. Goldschmidt, “Magnetic interactions in heavy atoms,” Phys. Lett. A 28, 265–266. (1968).
[Crossref]

Phys. Rev. (7)

B. R. Judd, “Three-particle operators for equivalent electrons,” Phys. Rev. 141, 4–14 (1966).
[Crossref]

B. R. Judd, H. M. Crosswhite, and H. Crosswhite, “Inter-atomic magnetic interactions for f electrons,” Phys. Rev. 169, 130–138 (1968).
[Crossref]

R. E. Trees, “Configuration interaction in Mn ii,” Phys. Rev. 83, 756–760 (1951); “Term values in the 3d54s configuration of Fe iii,” Phys. Rev. 84, 1089–1091 (1951).
[Crossref]

K. Rajnak and B. G. Wybourne, “Configuration interaction effects in lN configurations,” Phys. Rev. 132, 280–290 (1963).
[Crossref]

H. H. Marvin, “Mutual magnetic interactions of electrons,” Phys. Rev. 71, 102–110 (1947).
[Crossref]

G. Racah, “Theory of complex spectra. II,” Phys. Rev. 62, 438–462 (1942); “Theory of complex spectra. III,”  63, 367–382 (1943); “Theory of complex spectra. IV,”  76, 1352–1365 (1949).
[Crossref]

H. Crosswhite, H. M. Crosswhite, and B. R. Judd, “Magnetic parameters for the configuration f3,” Phys. Rev. 174, 89–94 (1968).
[Crossref]

Phys. Rev. A (4)

Z. B. Goldschmidt, “Spin-dependent interactions in U v 5f2,” Phys. Rev. A 27, 740–753 (1983).
[Crossref]

H. M. Crosswhite, “Effective electrostatic operators for two inequivalent electrons,” Phys. Rev. A 4, 485–489 (1971).
[Crossref]

J. Sugar and V. Kaufman, “Seventh spectrum of tungsten (W vii); resonance lines of Hf v,” Phys. Rev. A 12, 994–1012 (1975).
[Crossref]

J. C. Morrison, “Effect of core polarization upon the f–f interactions of rare-earth and actinide ions,” Phys. Rev. A 6, 643–650 (1972).
[Crossref]

Phys. Scr. (2)

J.-F. Wyart, V. Kaufman, and J. Sugar, “Analysis of the spectrum of four times-ionized uranium (U v),” Phys. Scr. 22, 389–396 (1980).
[Crossref]

J.-F. Wyart, J. Blaise, and P. Camus, “Progres récent dans l’interprétation des configurations 4fN(5d+ 6s) des lanthanides,” Phys. Scr. 9, 325–330 (1974).
[Crossref]

Physica (2)

P. F. A. Klinkenberg and R. Lang, “The spectrum of trebly ionized thorium, Th iv,” Physica 15, 774–788 (1949).
[Crossref]

P. F. A. Klinkenberg, “Analysis of double ionized thorium, Th iii,” Physica 16, 618–650 (1950); G. Racah, “On the spectrum of Th iii,” Physica 16, 651–666 (1950).
[Crossref]

Proc. K. Ned. Akad. Wet. (1)

H. Casimir, Proc. K. Ned. Akad. Wet. 34, 844 (1931).

Proc. R. Soc. Lond. Ser. A (1)

The Fischer program that we are using includes the Blume, Freeman, and Watson corrections to the spin–orbit integrals; see M. Blume and R. E. Watson, “Theory of spin–orbit coupling in atoms I. Derivation of the spin–orbit coupling constant,” Proc. R. Soc. Lond. Ser. A 270, 127–143 (1962); “II. Comparison of theory with experiment,” Proc. R. Soc. London Ser. 271, 565–578 (1963); M. Blume, A. J. Freeman, and R. E. Watson, “III.,” Phys. Rev. 134, A320–A327 (1964).
[Crossref]

Spectrochim. Acta Part B (1)

J. G. Conway, J. Blaise, and Jean Vergés, “The I.R. spectrum of curium-244,” Spectrochim. Acta Part B,  31, 31–47 (1976).
[Crossref]

Other (15)

A. Abragam and B. Bleaney, Electron Paramagnetic Resonance of Transition Ions (Clarendon, Oxford, 1970).

B. R. Judd, “Developments in atomic shell theory,” in The Structure of Matter, B. G. Wybourne, ed. (U. Canterbury Press, Christchurch, New Zealand, 1972); B. R. Judd and M. A. Suskin, “Complete set of orthogonal scalar operators for the configuration f3,” J. Opt. Soc. Am. B 1, 261–265 (1984).
[Crossref]

J. Blaise, Laboratoire Aimé Cotton, Orsay, France; J. G. Conway and E. Worden, Lawrence Livermore National Laboratory, Berkeley, California 94720 (personal communication).

These results are similar to those produced by R. D. Cowan’s HFR program. See Chap. 8 of his book.7

E. U. Condon and G. H. Shortley, The Theory of Atomic Spectra (Cambridge U. Press, Cambridge, 1935, 1951).

W. C. Martin, R. Zalubas, and L. Hagan, Atomic Energy Levels—The Rare-Earth Elements, NSRDS-NBS 60 (U.S. Government Printing Office, Washington, D.C., 1978).

U. Fano and G. Racah, Irreducible Tensorial Sets (Academic, New York, 1959).

B. R. Judd, Operator Techniques in Atomic Spectroscopy (McGraw-Hill, New York, 1963).

B. G. Wybourne, Spectroscopic Properties of Rare Earths (Interscience, New York, 1965).

Z. B. Goldschmidt, “Atomic properties (free atom),” in Handbook on the Physics and Chemistry of Rare Earths, K. A. Gschneidner and L. Eyring, eds. (North-Holland, Amsterdam, 1978), Vol. I, Chap. I, pp. 1–247.
[Crossref]

R. D. Cowan, The Theory of Atomic Structure and Spectra (U. California Press, Berkeley, Calif., 1981).

See, for instance, C. F. Fischer, The Hartree-Fock Method for Atoms (Wiley, New York, 1977).

G. H. Dieke, Spectra and Energy Levels of Rare Earths Ions in Crystals (Interscience, New York, 1966).

H. M. Crosswhite, “Systematic atomic and crystal-field parameters for lanthanides in LaCl3and LaF3,” in Spectroscopie des Éléments de Transition et des Éléments Lourdes dan Les Solides (Editions du CNRS, Paris, 1977), pp. 65–69.

S. Hüfner, Optical Spectra of Transparent Rare Earth Compounds (Academic, New York, 1978).

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Figures (4)

Fig. 1
Fig. 1

HF radial integrals F2(ff, ff) for lanthanide (solid curve) and actinide (dashed curve) fN configurations; experimental (Exp) F2 parameters for LaCl3 host for Ln3+ (○) and An3+ dopant (+) ions; and corresponding HF − experimental differences as a function of the number of electrons N.

Fig. 2
Fig. 2

Differences (ΔFk = HFR − experiment) between pseudo-relativistic HFR and experimental (Exp) values of the Slater parameters Fk, as determined from trivalent lanthanide ions in LaCl3 hosts.

Fig. 3
Fig. 3

Effective two-body electrostatic-operator parameters α, β and γ of lanthanide and actinide trivalent ions in LaCl3 and LaF3 hosts as a function of the number of electrons N.

Fig. 4
Fig. 4

Corrections to (top) Δξ = HFR − experiment pseudorelativistic HF calculations of spin–orbit and (bottom) spin–other-orbit parameters, as experimentally determined for trivalent lanthanides in the LaCl3 host.

Tables (10)

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Table 1 Experimental Parameters for Simple Configurations (in cm−1)

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Table 2 Corrections to HFR Calculations (Experimental − HFR Differences, in cm−1)

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Table 3 Effective-Operator Parameters for fN Configurations (in cm−1)

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Table 4 Parameters for Two-Body Magnetic Effective Operators (in cm−1)

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Table 5 Pr iii 4f3 Parameters for Magnetic Effective Operators (in cm−1)

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Table 6 Parameters for Three-body Electrostatic Effective Operators (in cm−1)

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Table 7 Zeta(d) Parameters (in cm−1)

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Table 8 Electrostatic fd-Parameter Differences (Exp. − HFR, in cm−1)

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Table 9 Electrostatic fd Effective-Operator Parameters (in cm−1)

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Table 10 Pseudomagnetic d-Electron Parameters (in cm−1)

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