The transient conductivity resulting from pulsed irradiation (with 3-MeV electrons) of a single, high-resistivity (4 {times} 10{sup 7} {Omega} m) crystal of CdS has been studied by nanosecond time-resolved microwave conductivity. The ratio of the electron-hole pair mobility to the pair formation energy is determined to be 42 {plus minus} 6 {times} 10{sup {minus}4} m{sup 2} V{sup {minus}1} s{sup {minus}1}/eV. For end-of-pulse pair concentrations less than ca. 10{sup 19} m{sup {minus}3}, the half-life of electrons toward localization was 25 ns. With increasing pair concentration above this value, the lifetime was found to become longer. This effect is attributed to trap saturation with the trap concentration estimated to be 3 {times} 10{sup 19} m{sup {minus}3} (5 {times} 10{sup {minus}8} M) with a rate constant toward trapping of 1.1 {times} 10{sup {minus}12} m{sup 3} s{sup {minus}1} (6.6 {times} 10{sup 14} M{sup {minus}1} s{sup {minus}1}). The main trapping site is thought to be the singly ionized sulfur vacancy. No evidence was found for the occurrence of direct electron-hole recombination, and an upper limit of 3 {times} 10{sup {minus}14} m{sup 3} s{sup {minus}1} (ca. 2 {times} 10{sup 13} M{sup {minus}1} s{sup {minus}1}) could be placed on the second-order rate constant for this process.
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