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Optical bistability in semiconductors
1.Both dispersive and absorptive optical bistability were first seen by H. M. Gibbs, S. L. McCall, and T. N. C. Venkatesan, Phys. Rev. Lett. 36, 1135 (1976).
2.T. N. C. Venkatesan and S. L. McCall, Appl. Phys. Lett. 30, 282 (1977);
2.S. L. McCall and H. M. Gibbs, J. Opt. Soc. Am. 68, 1378 (1978).
3.This follows immediately from Eq. (2) of Ref. 1.
4.H. M. Gibbs, A. C. Gossard, S. L. McCall, A. Passner, W. Wiegmann, and T. N. C. Venkatesan, Solid State Commun. 30, 271 (1979).
5.A. Szöke, V. Daneu, J. Goldhar, and N. A. Kurnit, Appl. Phys. Lett. 15, 376 (1969).
6.S. L. McCall and H. M. Gibbs (to be published).
6.Our inequality, Eq. (4), follows from Eq. (4) of Ref. 1 and the use of standard Bloch solutions, requiring that be somewhere negative for some detuning parameter. Inequality (3.2) of S. S. Hassan, P. D. Drummond, and D. F. Walls [Optics Comm. 27, 480 (1978)] is not enough to characterize bistability because their inequality can always be satisfied for some suitably large positive or negative detuning parameter.
7.H. M. Gibbs, T. N. C. Venkatesan, S. L. McCall, A. Passner, A. C. Gossard, and W. Wiegmann, Appl. Phys. Lett. 34, 511 (1979); CLEA 1979.
8.C. V. Shank, R. L. Fork, R. F. Leheny, and J. Shah, Phys. Rev. Lett. 42, 112 (1979).
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