Photonics and Lasers

Chapter 21 - CW Laser Characteristics

Chapter 21

 

CW Laser Characteristics

In the previous chapter, we considered the conditions under which lasing will occur. With steady-state pumping, there is a well-defined pump threshold, above which the intensity of laser light increases linearly with pump power. For some applications, it is not just the power of the laser light that is important but also its frequency spectrum. In this chapter, we consider the frequency distribution of laser light in the steady state. This is often referred to as continuous wave or CW operation. We explore the effect of gain saturation on the frequency spectrum, and consider ways in which the frequency can be stabilized or tuned over some range.

21-1. MODE SPECTRUM OF LASER LIGHT

 

In a laser cavity, the light intensity will build up to a high value only at the resonator mode frequencies, given by Eq. (16-3). Light in any of these modes will be amplified, provided that there is optical gain at the frequency of that mode. In order for lasing to occur in a given mode, the gain at that frequency must exceed or equal the threshold gain th. The number of modes that will lase, therefore, depends on how many modes have a gain th The number of modes with th will in turn depend on the way in which the gain curve saturates with intensity.

Single-mode Lasing

In our previous discussion of gain saturation, we assumed that all atoms were equivalent, having the same center frequency v0 . In this case, each atom saturates with intensity in the same way, and the gain curve is reduced by the same factor at each frequency v. This is referred to as homogeneous saturation, and is illustrated in Fig. 19-4a.

For steady-state operation, the value of (v) at any frequency v cannot exceed the threshold value th, because if it did the light intensity at that frequency would increase exponentially in time, and this would violate the assumption of steady-state operation. The gain curve (v) must, therefore, saturate so that the peak value is just at threshold, as shown in Fig. 21-1. Only the mode closest to the line center will lase in this case, since other modes will have < th. The result is single-mode lasing, with the output frequency spectrum as indicated in Fig. 21-1.

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