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Active laser medium
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===Efficiency of the gain medium=== The efficiency of a '''gain medium''' can be defined as <math>~ E =\frac{I_{\rm s} G}{I_{\rm p}A}~</math>. Within the same model, the efficiency can be expressed as follows: <math>~E =\frac{\omega_{\rm s}}{\omega_{\rm p}} \frac{1-V/p}{1+U/s}~</math>. For efficient operation, both intensities—pump and signal—should exceed their saturation intensities: <math>~\frac{p}{V}\gg 1~</math>, and <math>~\frac{s}{U}\gg 1~</math>. The estimates above are valid for a medium uniformly filled with pump and signal light. [[Spatial hole burning]] may slightly reduce the efficiency because some regions are pumped well, but the pump is not efficiently withdrawn by the signal in the nodes of the interference of counter-propagating waves.
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