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Passive (self‐pumped) phase conjugate mirror: Theoretical and experimental investigation
1.J. O. White, M. Cronin‐Golomb, B. Fischer, and A. Yariv, Appl. Phys. Lett. 40, 450 (1982).
2.J. Feinberg, D. Heiman, A. R. Tanguay, Jr., and R. W. Hellwarth, J. Appl. Phys. 51, 1297 (1980).
3.B. Fischer, M. Cronin‐Golomb, J. O. White, A. Yariv, and R. Neurgaonkar, Appl. Phys. Lett. 40, 863 (1982).
4.M. Cronin‐Golomb, B. Fischer, J. Nilsen, J. O. White, and A. Yariv, Appl. Phys. Lett. 41, 219 (1982).
5.For a review, see V. L. Vinetskii, N. V. Kukhtarev, S. G. Odulov, and M. S. Soskin, Usp. Fiz. Nauk, 129, 113 (1979)
5.[V. L. Vinetskii, N. V. Kukhtarev, S. G. Odulov, and M. S. Soskin, Sov. Phys. Usp. 22, 742 (1979)].
6.M. Cronin‐Golomb, B. Fischer, J. O. White, and A. Yariv, Opt. Lett. 7, 313 (1982).
7.This coupling strength depends on parameters such as crystal orientation electro‐optic tensor, and index grating wave vector [see B. Fischer, M. Cronin‐Golomb, J. O. White, and A. Yariv, Opt. Lett. 6, 519 (1981)]. When it is real, the phase shift between the light interference pattern and the refractive index grating is This is a behavior typical of photorefractive materials with no bias field. When is purely imaginary, the index grating is in phase with the light interference pattern, which is the case in media which have a local response such as atomic vapors.
8.This crystal measured and was poled into a single domain so that the c axis was parallel to the 4‐mm side.
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