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  1. E. Meinders and P. F. A. Klinkenberg, Physica 38, 253 (1968).
    [Crossref]
  2. Claire Arnoult and Simon Gerstenkorn, J. Opt. Soc. Am. 56, 177 (1966).
    [Crossref]
  3. K. H. Chan and P. J. Unsworth (private communication, 1966).
  4. J. M. Baker, J. R. Chadwick, G. Garton, and J. P. Hurrell, Proc. Roy. Soc. (London) 286, 352 (1965).
    [Crossref]
  5. A typographical error was apparently made in the eigenvector of the 8G5/2 level at 2889 cm−1. The component of 8G must be +0.851 rather than the −0.851 given. With the + sign, the eigenvector is orthogonal to the other J=52 states and is consistent with the observed hfs A and B values, as discussed in the letter.
  6. The A and B values of the states 8G15/2, 13/2, 11/2 are given to very high precision by Chan and Unsworth. The data obtained in the present determination of the g factors are consistent with their values of the A and B factors to within our 1% uncertainty.
  7. P. G. H. Sandars and J. Beck, Proc. Roy. Soc. (London) A289, 97 (1965).
  8. I. Bender, S. Penselin, and K. Schlupmann, Z. Physik 179, 4 (1964).
    [Crossref]

1968 (1)

E. Meinders and P. F. A. Klinkenberg, Physica 38, 253 (1968).
[Crossref]

1966 (1)

1965 (2)

J. M. Baker, J. R. Chadwick, G. Garton, and J. P. Hurrell, Proc. Roy. Soc. (London) 286, 352 (1965).
[Crossref]

P. G. H. Sandars and J. Beck, Proc. Roy. Soc. (London) A289, 97 (1965).

1964 (1)

I. Bender, S. Penselin, and K. Schlupmann, Z. Physik 179, 4 (1964).
[Crossref]

Arnoult, Claire

Baker, J. M.

J. M. Baker, J. R. Chadwick, G. Garton, and J. P. Hurrell, Proc. Roy. Soc. (London) 286, 352 (1965).
[Crossref]

Beck, J.

P. G. H. Sandars and J. Beck, Proc. Roy. Soc. (London) A289, 97 (1965).

Bender, I.

I. Bender, S. Penselin, and K. Schlupmann, Z. Physik 179, 4 (1964).
[Crossref]

Chadwick, J. R.

J. M. Baker, J. R. Chadwick, G. Garton, and J. P. Hurrell, Proc. Roy. Soc. (London) 286, 352 (1965).
[Crossref]

Chan, K. H.

K. H. Chan and P. J. Unsworth (private communication, 1966).

Garton, G.

J. M. Baker, J. R. Chadwick, G. Garton, and J. P. Hurrell, Proc. Roy. Soc. (London) 286, 352 (1965).
[Crossref]

Gerstenkorn, Simon

Hurrell, J. P.

J. M. Baker, J. R. Chadwick, G. Garton, and J. P. Hurrell, Proc. Roy. Soc. (London) 286, 352 (1965).
[Crossref]

Klinkenberg, P. F. A.

E. Meinders and P. F. A. Klinkenberg, Physica 38, 253 (1968).
[Crossref]

Meinders, E.

E. Meinders and P. F. A. Klinkenberg, Physica 38, 253 (1968).
[Crossref]

Penselin, S.

I. Bender, S. Penselin, and K. Schlupmann, Z. Physik 179, 4 (1964).
[Crossref]

Sandars, P. G. H.

P. G. H. Sandars and J. Beck, Proc. Roy. Soc. (London) A289, 97 (1965).

Schlupmann, K.

I. Bender, S. Penselin, and K. Schlupmann, Z. Physik 179, 4 (1964).
[Crossref]

Unsworth, P. J.

K. H. Chan and P. J. Unsworth (private communication, 1966).

J. Opt. Soc. Am. (1)

Physica (1)

E. Meinders and P. F. A. Klinkenberg, Physica 38, 253 (1968).
[Crossref]

Proc. Roy. Soc. (London) (2)

P. G. H. Sandars and J. Beck, Proc. Roy. Soc. (London) A289, 97 (1965).

J. M. Baker, J. R. Chadwick, G. Garton, and J. P. Hurrell, Proc. Roy. Soc. (London) 286, 352 (1965).
[Crossref]

Z. Physik (1)

I. Bender, S. Penselin, and K. Schlupmann, Z. Physik 179, 4 (1964).
[Crossref]

Other (3)

A typographical error was apparently made in the eigenvector of the 8G5/2 level at 2889 cm−1. The component of 8G must be +0.851 rather than the −0.851 given. With the + sign, the eigenvector is orthogonal to the other J=52 states and is consistent with the observed hfs A and B values, as discussed in the letter.

The A and B values of the states 8G15/2, 13/2, 11/2 are given to very high precision by Chan and Unsworth. The data obtained in the present determination of the g factors are consistent with their values of the A and B factors to within our 1% uncertainty.

K. H. Chan and P. J. Unsworth (private communication, 1966).

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Tables (1)

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Table I Observed hyperfine-interaction constants and gJ values in 159Tb. The figure in parentheses gives the uncertainty in the least significant figure for each value of A, B, and gJ.