Time-resolved spectroscopic measurements were made of the decay of a laser-produced discharge in hydrogen over a range of pressures from one to 70 atmospheres. The plasma temperature, which ranged from about 10
5to

K during the

-switched laser pulse to several microseconds afterward, was obtained from the ratio of the intensity of H
αto that of nearby continuum radiation. The electron density, which ranged from about 10
19to 10
17per cm
3was obtained from the time history of the Stark linewidths of H
αSince the high collision rates ensure approximate local thermodynamic equilibrium, several important characteristics of the plasma could be calculated from the measured temperature and density, such as optical absorption at the laser frequency due to inverse bremsstrahlung and photoionization. The energy deposited by the laser was measured from the decrease of the transmitted laser beam. Scattered radiation seemed small. The observed laser absorption is about two orders of magnitude larger than that calculated for a Maxwellian electron distribution. The calculated line absorption for H
αwas consistent with self-absorption observed in the H
αspectral profile. The ratio of the measured watts of H
αto the calculated watts/cm
3yielded values for the volume of the luminous region which generally decreased with gas pressure from 10
-3to 10
-4cm
3, as observed.