Abstract

From an analysis of the isotope shifts in the Cd 3261, 4678, and 4416 Å lines, it is pointed out that a precise determination of the odd–even staggering parameter is limited less by experimental error than by the lack of reliable knowledge of the specific mass effect.

© 1976 Optical Society of America

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References

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  1. J. M. Gagné and J. P. Saint-Dizier, J. Opt. Soc. Am. 65, 962 (1975).
    [Crossref]
  2. E. C. Woodward and D. R. Speck, Phys. Rev. 96, 529 (1954).
    [Crossref]
  3. S. Gerstenkorn, J. M. Helbert, and R. Lecordier, Phys. Lett. A 40, 229 (1972).
    [Crossref]
  4. C. Brechignac, Phys. Scr., 1975 (to be published).
  5. R. J. Hull and H. H. Stroke, J. Opt. Soc. Am. 53, 1147 (1963).
    [Crossref]

1975 (1)

1972 (1)

S. Gerstenkorn, J. M. Helbert, and R. Lecordier, Phys. Lett. A 40, 229 (1972).
[Crossref]

1963 (1)

1954 (1)

E. C. Woodward and D. R. Speck, Phys. Rev. 96, 529 (1954).
[Crossref]

Brechignac, C.

C. Brechignac, Phys. Scr., 1975 (to be published).

Gagné, J. M.

Gerstenkorn, S.

S. Gerstenkorn, J. M. Helbert, and R. Lecordier, Phys. Lett. A 40, 229 (1972).
[Crossref]

Helbert, J. M.

S. Gerstenkorn, J. M. Helbert, and R. Lecordier, Phys. Lett. A 40, 229 (1972).
[Crossref]

Hull, R. J.

Lecordier, R.

S. Gerstenkorn, J. M. Helbert, and R. Lecordier, Phys. Lett. A 40, 229 (1972).
[Crossref]

Saint-Dizier, J. P.

Speck, D. R.

E. C. Woodward and D. R. Speck, Phys. Rev. 96, 529 (1954).
[Crossref]

Stroke, H. H.

Woodward, E. C.

E. C. Woodward and D. R. Speck, Phys. Rev. 96, 529 (1954).
[Crossref]

J. Opt. Soc. Am. (2)

Phys. Lett. A (1)

S. Gerstenkorn, J. M. Helbert, and R. Lecordier, Phys. Lett. A 40, 229 (1972).
[Crossref]

Phys. Rev. (1)

E. C. Woodward and D. R. Speck, Phys. Rev. 96, 529 (1954).
[Crossref]

Other (1)

C. Brechignac, Phys. Scr., 1975 (to be published).

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Tables (1)

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TABLE I Staggering parameters, S, in cadmium, obtained in different transitions. Note that no errors are quoted because of the lack of knowledge of the specific mass shift, which may exceed by far the experimental errors. The values of the specific mass effects, K, given in the table, have been chosen to give a consistent set of S 63 .

Equations (2)

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S N + 1 = ( δ σ N + 1 , N + 2 - 1 2 δ σ N , N + 2 ) / ( 1 2 δ σ N , N + 2 ) .
( S N + 1 ) exp = ( δ σ N + 1 , N + 2 - 1 2 δ σ N , N + 2 ) / ( 1 2 δ σ N , N + 2 + K ) ,