Abstract
Picosecond infrared techniques have been used to probe the time‐varying transmission and reflection coefficients at 10.6 μm of a nonequilibrium electron‐hole gas in Hg1−xCdxTe (x = 0.3 and 0.2) at peak densities of approximately 1×1019 cm−3. Observed recombination times are much longer than those predicted by extrapolations based on conventional theory of Auger recombination in the nondegenerate density regime.
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