Optical Nonlinearities in LiIO3
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4.S. K. Kurtz and T. T. Perry, J. Appl. Phys. 39, 3798 (1968). There is a misprint in parts (c) and (d) of the appendix in this paper. (114/105) should be replaced by (101/105).
5.The dip in Fig. 1 at is of unknown origin.
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13.Reference 11, Chap. XIV.
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17.One method which measures the index and is suitable for very small crystals is based upon a modification of a technique introduced by the Duke of Chaulnes. A similar procedure employing a different averaging technique has been used by A. Miller, J. Opt. Soc. Amer. 58, 428 (1968). Our values for the indices and the birefringence agreed to within 3% with the more accurate results of Ref. 16. In establishing these values we used our measured indices at 0.59 μ, the relationship between the phase matching angle and the indices (Appendix), the coherence lengths (Sec. 5) and we assumed that in the immediate vicinity of any wavelength the dispersion in was identical to that in Ref. 1. We also measured B directly using an Ehringhaus compensator and polarizing microscope. The value found is somewhat suspect because it has been noted by several researchers at Bell Telephone Laboratories that this technique consistently gives a value of B for which is too large by
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23.A prism with one face coated as an output flat was used to discriminate against unwanted transitions in the laser. The output Gaussian beam had a measured radius which was ∼30% smaller than that calculated. For the purposes of data reduction the beam radius at the crystal was measured.
24.R. C. Miller, G. D. Boyd, and A. Savage, Appl. Phys. Lett. 6, 77 (1965). This observation is supported by the fact that in a direct observation of birefringence, no change was observed with a 100 °C increase in crystal temperature.
25.J. E. Bjorkholm, Phys. Rev. 142, 126 (1966).
26.The f functions of and are equivalent to G(t, 0) for There is a plot of G(t, 0) in for and for all t in with asymptotic expansions in Eq. (2.40).
27.The significant quantity in nonlinear experiments is the value of If the assumption of negligible ρ had been preserved our estimate of for would have been 20% too high.
28.J. E. Bjorkholm, IEEE J. Quantum Electron. 4, 970 (1968);
28.J. E. Bjorkholm, 5, 260 (1969)., IEEE J. Quantum Electron.
29.M. Born and E. Wolf, Principles of Optics (Pergamon Press, Inc., New York, 1959), Chap. 1.5, Eq. (35).
30.F. Zernike, Jr., J. Opt. Soc. Amer. 54, 1215 (1964).
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36.I. P. Kaminow and E. H. Turner, Proc. IEEE 54, 1374 (1966).
37.Reference 29, p. 677.
38.J. A. Giordmaine, Phys. Rev. Lett. 8, 19 (1962).
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