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Topical Meeting on Optical Bistability (OB)

Stability of a 2-photon bistable system in a standing wave cavity

S. M. A. Maize, B. V. Thompson, Saad S. M. Hassan

Published Jan 1, 1985• 0 citations
Publisher

Abstract

In the one photon OB problem, McCalls method [1] gives an accurate solution for the stationary behaviour of the forward and backward field envelopes while the Fleck approach [2] has serious faults [3,4]. A linear stability analysis using truncation [5] predicts instabilities of self-pulsing type on the upper transmission branch for C > 60 (C is the cooperation parameter). We have repeated this investigation but using McCall’s method in order to test how useful the truncation method is for time dependent problems. We find that the upper branch is now stable for several values of C > 60.

DOI
10.1364/obi.1985.md3

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Physical Review A•Mar 1, 1986•8 citations
In the one photon OB problem, McCalls method [1] gives an accurate solution for the stationary behaviour of the forward and backward field envelopes while the Fleck approach [2] has serious faults [3,4]. A linear stability analysis using truncation [5] predicts instabilities of self-pulsing type on the upper transmission branch for C > 60 (C is the cooperation parameter). We have repeated this investigation but using McCall’s method in order to test how useful the truncation method is for time dependent problems. We find that the upper branch is now stable for several values of C > 60.
We review and extend the theory of instabilities in absorptive optical bistability for ring cavities containing homogeneously broadened two-level media. The instabilities occur in the high-transmission branch and result in either a precipitation to the low-transmission branch or in pulsed multimode operation. Two numerical approaches are used to predict operation away from the simple mean-field limit. First, an iterative method is used to solve the general field eigenvalue equation for cavity modes with frequencies displaced from the input frequency. This work shows that the instability region decreases in size as the mirror transmission increases. These calculations are confirmed by the second numerical technique, consisting of direct integrations of the coupled Maxwell-Bloch equations. This second approach also provides time histories of the instability evolutions, and divides the instability range into a precipitation regime and a self-pulsing regime. The results are discussed in terms of first- and second-order phase transitions, and agree with the analytical results obtained within the dressed-mode description of optical bistability. They show that when the incident field is adiabatically decreased along the high-transmission branch, the spiking behavior always appears abruptly. By further decreasing the incident intensity, the self-pulsing disappears either continuously if the system remains in the high-transmission branch, or discontinuously if the system precipitates to the low-transmission branch. Connection is made with induced probe gain known in the saturation spectroscopy of absorbers (uninverted media), in which population pulsations transfer energy from a saturating wave to the probe waves. The very close relationship with multimode operation in homogeneously broadened unidirectional ring lasers is also established.
A semiclassical theoretical model is described under the plane-wave and mean-field approximations on the transmission characteristics of a system of two-level atoms with large permanent dipole moments contained in a Fabry-Perot cavity and driven by two coherent two-photon resonant fields. In the steady-state situation, the coupled field equations are solved by eliminating one of the field variables to obtain the state equation. This state equation is numerically analyzed in detail, thus providing the regions on two-dimensional maps corresponding to one, three, and five stationary states of the system. The linear stability analysis is also carried out for the case when the length of the cavity is such that the medium-relaxation times are much shorter than the cavity-photon life times for both the waves. The simple stability criterion that the negative-slope regions of the transmission curves are unstable holds, but only the lowest positive-slope branches show stability in all of the cases we tested numerically.
The static criterion for multiphoton optical bistability in a high-Q ring cavity is analytically derived for a homogeneously broadened atomic system when the input coherent field is in perfect resonance with the atoms and with the cavity. It is shown how the static threshold condition, the bistable regime, the critical point, and the threshold input field amplitude for the optical bistability, change with the variables of the photon number involved in the transition and the system parameter C/sub n/. Criteria for the stability of the stationary solutions are derived and discussed. The results show that in the input-output curves, all parts of the branches with negative slope are unstable, and some parts of the branches with positive slope may be unstable. Considering the stability of the stationary solutions, complete criteria for optical bistability are discussed.>
This chapter concludes the discussion about temporal instabilities and self-oscillations, considering the instabilities that arise in the systems analyzed in Chapter 13, with the exception of optical bistability, which has been discussed separately in Chapter 11. Section 25.1 focuses on the laser with an injected signal. As already mentioned in Section 13.1, in this system self-pulsing instabilities are rather ubiquitous, and on exploring the parameter space one meets an extremely rich variety of oscillatory behaviors. For example, under extremely high-gain conditions, breathing, spiking and chaos have been identified over various ranges of the driving field strength [294]. In this section we show some results that arise under parametric conditions that are more accessible experimentally. We illustrate especially the coexistence, for the same parametric values, of different oscillatory behaviors that are reached by starting from different initial conditions. On the other hand, Section 25.2 deals with a laser with a saturable absorber. In this system even the full scenario of stationary intensity solutions in the single-mode model is very complex. For the sake of simplicity, in this section we focus on a simpler rate-equation model that is obtained from the single-mode model of Eqs. (13.13)–(13.17) by adiabatically eliminating the atomic polarization of both active and passive medium. As in Chapter 13, we assume that the atomic transition frequencies are equal and also coincide with a cavity frequency. In this way all the variables in the model can be assumed real, and the linearization around the stationary solution described in Section 13.2 leads to a cubic eigenvalue equation. The spontaneous oscillations which arise from this instability are called repetitive passive Q-switching in the literature. Section 25.3 considers the stability of the stationary solutions of the degenerate optical parametric oscillator described in Section 13.4 and outlines the scenario of period doubling and chaos that arises under appropriate parametric conditions.
The general ring cavity optically bistable systems with two partially reflecting mirrors of unequal transmissivity are analysed. In the mean field approximation, the steady state equation is given, and the linear stability analysis of the steady states is performed. It is found that when the ratio of transmissivity T_1/T_2 varies, the bistable loop changes its size and even the systematic behavior varies from the bistability mode into the amplification mode. It is pointed out that in the mean field approximation there are many systems with (?)≡CT_1/L_v(?)1 and also many systems with (?)1. The self-pulsing instability is observed in the latter systems.
We study the semiclassical mean-field theory of single-mode dispersive optical bistability in the limit of a fully developed hysteresis cycle (i.e., in the limit of large values of the bistability parameter C) and when all decay rates have comparable magnitude. We locate (i) on the upper branch instabilities leading to time periodic regimes, (ii) on the lower branch instabilities leading to a switching before the limit point is reached. None of these instabilities are observed in the case of purely absorptive optical bistability.