Abstract

New and very accurate data of isotope shifts and relative isotope shifts in 234U, 236U, 238U are presented. The invariance of the relative isotope shift, for the transitions we have investigated, supports the hypothesis that the so-called specific mass effect is negligible in uranium.

© 1976 Optical Society of America

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References

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  1. J. M. Gagné, J. M. Helbert, and S. Gerstenkorn, C. R. Acad. Sci. 259, 3479 (1964).
  2. S. Gerstenkorn, J. Phys. C T-34, 55 (1973).
  3. R. Chabbal and P. Jacquinot, Rev. Opt. 40, 157 (1961).
  4. J. M. Gagné, M. Giroux, and J. P. Saint-Dizier, Appl. Opt. 12, 522 (1973).
    [Crossref]
  5. J. M. Gagné, J. P. Saint-Dizier, and M. Picard, App. Opt. 13, 581 (1974).
    [Crossref]
  6. F. Guyon, J. Blaise, and J. F. Wyart, J. Phys. T. 35, 929 (1974).
    [Crossref]
  7. M. Diringer, Ann. Phys. 10, 89 (1965).
  8. P. Brix and H. Kopfermann, Z. Phys. 126, 344 (1949).
    [Crossref]
  9. H. Kopfermann, Nuclear Moments (Academic, New York, 1958).
  10. J. Bauche, J. Phys. T.35, 19 (1974).

1974 (3)

J. M. Gagné, J. P. Saint-Dizier, and M. Picard, App. Opt. 13, 581 (1974).
[Crossref]

F. Guyon, J. Blaise, and J. F. Wyart, J. Phys. T. 35, 929 (1974).
[Crossref]

J. Bauche, J. Phys. T.35, 19 (1974).

1973 (2)

1965 (1)

M. Diringer, Ann. Phys. 10, 89 (1965).

1964 (1)

J. M. Gagné, J. M. Helbert, and S. Gerstenkorn, C. R. Acad. Sci. 259, 3479 (1964).

1961 (1)

R. Chabbal and P. Jacquinot, Rev. Opt. 40, 157 (1961).

1949 (1)

P. Brix and H. Kopfermann, Z. Phys. 126, 344 (1949).
[Crossref]

Bauche, J.

J. Bauche, J. Phys. T.35, 19 (1974).

Blaise, J.

F. Guyon, J. Blaise, and J. F. Wyart, J. Phys. T. 35, 929 (1974).
[Crossref]

Brix, P.

P. Brix and H. Kopfermann, Z. Phys. 126, 344 (1949).
[Crossref]

Chabbal, R.

R. Chabbal and P. Jacquinot, Rev. Opt. 40, 157 (1961).

Diringer, M.

M. Diringer, Ann. Phys. 10, 89 (1965).

Gagné, J. M.

J. M. Gagné, J. P. Saint-Dizier, and M. Picard, App. Opt. 13, 581 (1974).
[Crossref]

J. M. Gagné, M. Giroux, and J. P. Saint-Dizier, Appl. Opt. 12, 522 (1973).
[Crossref]

J. M. Gagné, J. M. Helbert, and S. Gerstenkorn, C. R. Acad. Sci. 259, 3479 (1964).

Gerstenkorn, S.

S. Gerstenkorn, J. Phys. C T-34, 55 (1973).

J. M. Gagné, J. M. Helbert, and S. Gerstenkorn, C. R. Acad. Sci. 259, 3479 (1964).

Giroux, M.

Guyon, F.

F. Guyon, J. Blaise, and J. F. Wyart, J. Phys. T. 35, 929 (1974).
[Crossref]

Helbert, J. M.

J. M. Gagné, J. M. Helbert, and S. Gerstenkorn, C. R. Acad. Sci. 259, 3479 (1964).

Jacquinot, P.

R. Chabbal and P. Jacquinot, Rev. Opt. 40, 157 (1961).

Kopfermann, H.

P. Brix and H. Kopfermann, Z. Phys. 126, 344 (1949).
[Crossref]

H. Kopfermann, Nuclear Moments (Academic, New York, 1958).

Picard, M.

J. M. Gagné, J. P. Saint-Dizier, and M. Picard, App. Opt. 13, 581 (1974).
[Crossref]

Saint-Dizier, J. P.

J. M. Gagné, J. P. Saint-Dizier, and M. Picard, App. Opt. 13, 581 (1974).
[Crossref]

J. M. Gagné, M. Giroux, and J. P. Saint-Dizier, Appl. Opt. 12, 522 (1973).
[Crossref]

Wyart, J. F.

F. Guyon, J. Blaise, and J. F. Wyart, J. Phys. T. 35, 929 (1974).
[Crossref]

Ann. Phys. (1)

M. Diringer, Ann. Phys. 10, 89 (1965).

App. Opt. (1)

J. M. Gagné, J. P. Saint-Dizier, and M. Picard, App. Opt. 13, 581 (1974).
[Crossref]

Appl. Opt. (1)

C. R. Acad. Sci. (1)

J. M. Gagné, J. M. Helbert, and S. Gerstenkorn, C. R. Acad. Sci. 259, 3479 (1964).

J. Phys. (1)

J. Bauche, J. Phys. T.35, 19 (1974).

J. Phys. C (1)

S. Gerstenkorn, J. Phys. C T-34, 55 (1973).

J. Phys. T. (1)

F. Guyon, J. Blaise, and J. F. Wyart, J. Phys. T. 35, 929 (1974).
[Crossref]

Rev. Opt. (1)

R. Chabbal and P. Jacquinot, Rev. Opt. 40, 157 (1961).

Z. Phys. (1)

P. Brix and H. Kopfermann, Z. Phys. 126, 344 (1949).
[Crossref]

Other (1)

H. Kopfermann, Nuclear Moments (Academic, New York, 1958).

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Figures (1)

FIG. 1
FIG. 1

Example of recording of an even isotope line profile with the refractometer reference interferogram.

Tables (2)

Tables Icon

TABLE I Experimental isotope shift values in Ui.

Tables Icon

TABLE II Relative isotope shift in Ui.

Equations (3)

Equations on this page are rendered with MathJax. Learn more.

Δ σ α β a = K α A α β + E α C α β ,
A α β = ( A β - A α ) / A β A α ,
( RIS a RIS b ) exp Δ σ α β a / Δ σ α β a Δ σ α β b / Δ σ α β b 1