Abstract
When using a nonlinear medium in a Fabry-Perot interferometer (F.P.), optical bistability is due to an intensity dependence of the real or imaginary part of the dielectric function1,2.
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References
H.M. Gibbs, S.L. McCall and T.N.C. Venkatesan, Differential Gain and Bistability using a Sodium-Filled Fabry-Perot Interferometer, Phys. Rev. Letters, 36:1135 (1976).
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R. Levy, J.Y, Bigot, B. Hönerlage, F. Tomasini and J.B, Grun, Optical Bistability Due to Biexcitons in CuCl, to be published.
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© 1984 Plenum Press, New York
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Hönerlage, B., Bigot, JY., Levy, R. (1984). Optical Bistability in CuCl. In: Bowden, C.M., Gibbs, H.M., McCall, S.L. (eds) Optical Bistability 2. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-4718-7_36
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DOI: https://doi.org/10.1007/978-1-4684-4718-7_36
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