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Journal of the Optical Society of America A

Observation of the single-mode instability in optical bistability (A)

Luis A. Orozco, Albert T. Rosenberger, Harry J. Kimble

Published Jan 1, 1984• 1 citation
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Related papers

Experimental Investigation of the Single-Mode Instability in Optical Bistability

Albert T. Rosenberger, Luis A. Orozco, Harry J. Kimble

NATO ASI series. Series B : Physics•Jan 1, 1988•0 citations

Observation of the Single-Mode Instability in Optical Bistability

Albert T. Rosenberger, Luis A. Orozco, Harry J. Kimble

The effect of transverse intensity variation on the various instabilities associated with optical bistability seems to be catastrophic in the case of pure absorptive bistability1,2 but benign in the mixed absorptive-dispersive case.2,3 In particular, recent results of Lugiato et al.2 indicate that the mean-field single-mode instability is not destroyed by the assumption of a Gaussian transverse intensity profile, and that it should be observable for experimentally accessible parameter values. Stimulated by these results, we have looked for and observed self-pulsing due to the single-mode instability in the predicted region of parameter space.

•Jun 18, 1984•1 citation

Dynamical aspects in optical bistability

Luigi A. Lugiato, Franco Prati, Massimo Brambilla

Although the discovery of oscillatory instabilities (both single-mode and multimode) in free-running lasers was achieved in the 1960s, investigations on oscillatory instabilities in optical bistability did not take place until the 1970s and 1980s. The first section of this chapter does not deal with oscillatory instabilities, but instead concerns an interesting dynamical phenomenon in optical bistability that arises when the input field approaches a boundary of the bistable domain, and is called critical slowing down . This has been investigated both theoretically and experimentally. The remainder of this chapter is entirely devoted to oscillatory instabilities, following a historical order. With an inverse approach with respect to the laser case, we discuss multimode instabilities first. In Section 24.2.1 we start with the description of the instability which arises under exactly resonant conditions. While this is the counterpart in optical bistability of the resonant multimode laser instability discussed in Section 22.5, a striking difference from the laser case is that in the passive configuration there is no corresponding single-mode instability. This difference disappears, however, when we consider the generalization of the multimode instability of optical bistability to the detuned configuration. Finally we show that in the detuned case it has been possible to achieve a convincing experimental observation of the multimode instability in a long microwave cavity. After some relevant miscellaneous considerations in Section 24.2.2, in Section 24.2.3 we address the subject of the multimode Ikeda instability which leads to period doubling and chaos and aroused a lot of interest in optical chaos. We emphasize also the intrinsic connections with the standard multimode instability discussed in Section 24.2.1, showing, in particular, that the Ikeda instability requires conditions far from the low-transmission limit, i.e. that ∝L is not small. In Section 24.3 we discuss single-mode instabilities in optical bistability. In Section 24.3.1 we illustrate a configuration for the single-mode instability that includes also the Gaussian shape of the electric field in the beam section, and leads to periodic, close-to-sinusoidal self-pulsations.

Cambridge University Press eBooks•Feb 28, 2015•0 citations

Quantitative test of the single-mode theory of optical bistability

Luis A. Orozco, Harry J. Kimble, Albert T. Rosenberger

Optics Communications•Apr 1, 1987•21 citations

Intrinsic Dynamical Instability in Optical Bistability with Two-Level Atoms

Luis A. Orozco, Albert T. Rosenberger, Harry J. Kimble

Self-pulsing instability is reported in an experiment in which two-level atoms couple to a single mode of a traveling-wave resonator to produce optical bistability. The threshold for the onset of oscillation together with the characteristics of the dynamical state are described. The self-pulsing instability observed is the analog in an absorbing system of the single-mode laser instability.

Physical Review Letters•Dec 31, 1984•69 citations

Optical Bistability and Its Instability

Chunfei Li

Nonlinear Optics•Aug 26, 2016•2 citations
The effect of transverse intensity variation on the various instabilities associated with optical bistability seems to be catastrophic in the case of pure absorptive bistability1,2 but benign in the mixed absorptive-dispersive case.2,3 In particular, recent results of Lugiato et al.2 indicate that the mean-field single-mode instability is not destroyed by the assumption of a Gaussian transverse intensity profile, and that it should be observable for experimentally accessible parameter values. Stimulated by these results, we have looked for and observed self-pulsing due to the single-mode instability in the predicted region of parameter space.
Although the discovery of oscillatory instabilities (both single-mode and multimode) in free-running lasers was achieved in the 1960s, investigations on oscillatory instabilities in optical bistability did not take place until the 1970s and 1980s. The first section of this chapter does not deal with oscillatory instabilities, but instead concerns an interesting dynamical phenomenon in optical bistability that arises when the input field approaches a boundary of the bistable domain, and is called critical slowing down . This has been investigated both theoretically and experimentally. The remainder of this chapter is entirely devoted to oscillatory instabilities, following a historical order. With an inverse approach with respect to the laser case, we discuss multimode instabilities first. In Section 24.2.1 we start with the description of the instability which arises under exactly resonant conditions. While this is the counterpart in optical bistability of the resonant multimode laser instability discussed in Section 22.5, a striking difference from the laser case is that in the passive configuration there is no corresponding single-mode instability. This difference disappears, however, when we consider the generalization of the multimode instability of optical bistability to the detuned configuration. Finally we show that in the detuned case it has been possible to achieve a convincing experimental observation of the multimode instability in a long microwave cavity. After some relevant miscellaneous considerations in Section 24.2.2, in Section 24.2.3 we address the subject of the multimode Ikeda instability which leads to period doubling and chaos and aroused a lot of interest in optical chaos. We emphasize also the intrinsic connections with the standard multimode instability discussed in Section 24.2.1, showing, in particular, that the Ikeda instability requires conditions far from the low-transmission limit, i.e. that ∝L is not small. In Section 24.3 we discuss single-mode instabilities in optical bistability. In Section 24.3.1 we illustrate a configuration for the single-mode instability that includes also the Gaussian shape of the electric field in the beam section, and leads to periodic, close-to-sinusoidal self-pulsations.