Photonics and Lasers

Chapter 18 - Stimulated Emission and Optical Gain

Chapter 18

 

Stimulated Emission and Optical Gain

In the previous three chapters, we considered the special properties of laser light, and the way a laser beam propagates both inside and outside of a laser cavity. The laser cavity provides optical feedback, and is one of the three major components of a laser. We now turn to a discussion of the second essential component, the gain medium. This is the material between the cavity mirrors that amplifies the light as it propagates back and forth between the mirrors. The amplification occurs by stimulated emission, which we briefly discussed in Chapter 15. In this chapter, we consider stimulated emission in more detail, and show how it is related to the gain coefficient of an optical amplifier or laser.

18-1. TRANSITION RATES

  Stimulated emission is one of the three fundamental processes by which an atom can make a radiative transition between two energy levels. As illustrated in Fig. 15-2, it occurs when a photon is incident on an atom that is initially in the upper of two energy levels. For stimulated emission to occur, the resonance condition hv = E21 must be satisfied, where hv is the photon energy and E21 = E2 E1 is the energy difference between the two levels. If the photon energy were perfectly well defined (monochromatic light) and the atomic transition energy were perfectly sharp (no uncertainty or spread in energy), there would be no stimulated emission (or absorption) unless the two happened to match up exactly, a rather rare occurance. In practice, there is always some width to both hv and E21, which allows stimulated emission to occur over a range of photon frequencies.

 

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