Abstract
Chapter 6 gives the theory of a laser, which is a self-sustained oscillator consisting of an active medium in a Fabry-Perot or ring cavity. The laser output frequencies, imposed by the self-consistent laser equations, are compromises between the atomic and cavity natural frequencies. In this chapter, we discuss another situation involving a nonlinear medium in Fabry-Perot and ring cavities, but with two major changes: 1) the cavity output depends on an injected signal for its energy and output frequency, and 2) the medium is passive, i.e., it absorbs and/or provides an index change — but for two-level media, the upper state is not pumped. The name optical bistability comes from the characteristic of such systems that for a single input intensity, two (or more) stable output intensities are often possible, one large and one small. The system is like an electronic flip-flop, except that it is all optical.
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References
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© 1990 Springer-Verlag Berlin Heidelberg
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Meystre, P., Sargent, M. (1990). Optical Bistability. In: Elements of Quantum Optics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-07007-9_7
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DOI: https://doi.org/10.1007/978-3-662-07007-9_7
Publisher Name: Springer, Berlin, Heidelberg
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