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ELECTRO‐OPTIC EFFECT AND MODULATED INTERFERENCE IN TANTALUM OXIDE FILMS
1.F. G. Ullman and B. J. Holden, Bull. Am. Phys. Soc. 12, 1132 (1967).
2.B. J. Holden and F. G. Ullman, J. Electrochem. Soc. 116, 280 (1969).
3.A. Frova and P. Migliorato, Appl. Phys. Letters 13, 328 (1968).
4.See, for instance, F. S. Chen, J. E. Geusic, S. K. Kurtz, and S. H. Wemple, J. Appl. Phys. 37, 388 (1966).
5.B. J. Holden and F. G. Ullman, Appl. Phys. Letters (to be published). The authors are indebted to Professor Ullman for bringing this paper to their attention prior to publication.
6.M. Born and E. Wolf, Principles of Optics, 3rd rev. ed. (Pergamon Press, New York, 1965), p. 632.
7.D. Gerstenberg, J. Electrochem. Soc. 113, 542 (1966).
8.S. Kumagai and L. Young, J. Electrochem. Soc. 111, 1411 (1964).
9.M. DiDomenico and S. H. Wemple, J. Appl. Phys. 40, 720 (1969).
10.See L. Young, Proc. Roy. Soc. (London) A244, 41 (1958), and references therein.
11.J. D. Zook and T. N. Casselman, Phys. Rev. Letters 17, 960 (1966).
12.In Ref. 3, by printer’s error, the factor has been omitted in the expression giving
13.The authors are grateful to S. H. Wemple for pointing out that, although in general one should consider a contribution from photoelastic effects, this does not change the form of Eq. (4), but might simply alter the coefficients β and K to some extent [see S. H. Wemple and M. DiDomenico, Jr., Phys. Rev. (to be published)]. That is, the β and K values obtained here may be appropriate for clamped crystal, undamped, or some intermediate situation.
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