Photolysis of HI dissolved in perdeuterated 3-methylpentane (3MP-di4) glass at any temperature from 4 to 50°K produces trapped H atoms and trapped D atoms observable by esr, as well as C6Di3 radicals formed by abstraction of D from the 3MP-di4 by hot H. CeH13 radicals, but no trapped H atoms, are produced by photolysis of HI in 3MP-/q4 under identical conditions, indicating a major effect of isotopic substitution on the trapping capability of the matrix. The initial quantum yield of trapped H in 3MP-cZi4 (ca. 0.03) is independent of temperature over the range of at least 20-40°K but decreases with time of photolysis until a steady-state concentration is reached, while the concentrations of CeDia and D continue to grow linearly. The fractional rate of decay of trapped H atoms following short illuminations decreases rapidly with time, but the decay curves for samples with different initial concentrations are superimposable after normalization for dose. The properties of trapped H produced in 3MP-d14 in Kel-F tubes are the same as when produced in quartz tubes. Trapped H atoms may be produced by photolysis of empty quartz tubes after certain conditions of aging and y radiolysis. Trapped D (or ) atoms are not produced by the radiolysis of 3MP-d44 (or 3MP-%i4) with or without dissolved HI present, although photolysis of HI in radiolyzed 3MP-di4 produces them. The implications of the data with respect to the mechanism of H atom trapping and decay are discussed.