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  1. E. Meinders and P. F. A. Klinkenberg, Physica 38, 253 (1968).
  2. Claire Arnoult and Simon Gerstenkorn, J. Opt. Soc. Am. 56, 177 (1966).
  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).
  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 = 5/2 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).

Arnoult, Claire

Claire Arnoult and Simon Gerstenkorn, J. Opt. Soc. Am. 56, 177 (1966).

Baker, J. M.

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

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).

Chadwick, J. R.

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

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).

Gerstenkorn, Simon

Claire Arnoult and Simon Gerstenkorn, J. Opt. Soc. Am. 56, 177 (1966).

Hurrell, J. P.

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

Klinkenberg, P. F. A.

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

Meinders, E.

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

Penselin, S.

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

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).

Unsworth, P. J.

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

Other (8)

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

Claire Arnoult and Simon Gerstenkorn, J. Opt. Soc. Am. 56, 177 (1966).

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

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

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 = 5/2 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.

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

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

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