# Gain Efficiency

Definition: small-signal gain of an optical amplifier per unit pump power or per unit stored energy

German: Verstärkungseffizienz

Categories: laser devices and laser physics, optical amplifiers

Units: dB/W, 1/W

Author: Dr. Rüdiger Paschotta

Cite the article using its DOI: https://doi.org/10.61835/3r6

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The gain efficiency of an amplifier can be defined as the small-signal gain divided by the pump power required to achieve this gain in the steady state. For three-level gain media, where the gain without pumping is negative, it is more sensible to use the *differential* gain efficiency, i.e. the derivative of the small-signal gain with respect to the pump power.

For pulsed operation, the gain efficiency may also sometimes refer to the stored energy instead of the pump power.

For a laser gain medium with emission and absorption cross-sections <$\sigma_\rm{em}$> and <$\sigma_\rm{abs}$> and photon energy <$h\nu$> at the signal wavelength, and a mode area <$A$> (assuming a flat-top profile), the dependence of the gain on the stored energy can be simply calculated as

$$\frac{{\partial g}}{{\partial {E_{{\rm{stored}}}}}} = \frac{{{\sigma _{{\rm{em}}}} + {\sigma _{{\rm{abs}}}}}}{{h{v_{\rm{p}}}\;A}} = \frac{1}{{{E_{{\rm{sat}}}}}}$$where the power amplification factor is <$\exp(g)$>. (For a four-level gain medium, <$\sigma_\rm{abs}$> = 0.) This shows that the gain efficiency in terms of stored energy is inversely related to the saturation energy: high laser cross-sections lead to a high gain efficiency, but also to a low saturation energy.

The pump power required for achieving a certain stored energy in the steady state depends on the upper-state lifetime of the laser transition: the shorter this lifetime, the higher is the rate with which ions needs to be pumped into the upper laser level. For the differential gain efficiency in terms of pump power, this leads to the equation

$$\frac{{\partial g}}{{\partial {P_{\rm{p}}}}} = {\eta _{\rm{p}}}{\tau _2}\frac{{\partial g}}{{\partial {E_{{\rm{stored}}}}}} = {\eta _{\rm{p}}}\frac{{{\tau _2}\left( {{\sigma _{{\rm{em}}}} + {\sigma _{{\rm{abs}}}}} \right)}}{{h{v_{\rm{p}}}\;A}} = \frac{{{\eta _{\rm{p}}}}}{{{P_{{\rm{sat}}}}}}$$where <$\eta_\textrm{p}$> is the pump efficiency, including the pump absorption efficiency, the quantum efficiency of the pumping process, and the quantum defect. <$P_\rm{sat}$> is the saturation power, which is the saturation energy divided by the upper-state lifetime.

Fiber amplifiers with small effective mode area can easily reach differential gain efficiencies of several dB/mW, with special optimization even more than 10 dB/mW. A high gain efficiency can be desirable for an amplifier when a high gain is wanted. However, it can be preferable to have a not too large gain efficiency in cases where a high energy needs to be stored in a gain medium – for example for Q switching of a laser, or if pulses need to be amplified to high energies.

The gain efficiency should not be confused with the power conversion efficiency. For example, an optical amplifier based on a laser crystal may have a low gain efficiency (due to a large mode area) but nevertheless a high power conversion efficiency.

See also: gain, saturation energy, optical amplifiers, spotlight 2007-05-10

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