Distributed Feedback Semiconductor Lasers

Push ?pull operation is well known in electronics where, for example (Figure 8.9), a pair of transistors T 1 and T 2 are coupled at their emitters (marked E). Because of a sufficiently large resistance R t ('the long tail') there is a constant current I flowing equally between the two transistors in the steady state. On driving the input (the base of T 1) positive, the current in T1, is enhanced by ? I but, because of the constant-current source at the coupled emitters, the current into T 2 is reduced by ? I. The base at transistor T 2 is shown to be fixed at 'ground' potential but could equally well have been driven by a second input provided that the polarity was opposite to that at the base input of T 1. The ' push-pull' outputs are then capable of driving another similar circuit. This circuit is a remarkably high-speed circuit because both transistors are operated with either unity voltage gain or unity current gain which then gives the potential for working at the limit of their gain-bandwidth product signified by the transition frequency f t. The emitter E is the output for the first transistor (T 1) for driving transistor T 2. Consequently, the transistor T 1 is effectively operated as an emitter follower with unity voltage gain. The transistor T