Abstract
Time‐domain experiments on the OCS J=0−1 ΔM=0 microwave transition have been used to measure the pressure dependence of two relaxation times: for radiation from a coherently excited sample, 1/T2=37.66±0.10 μsec−1⋅Torr−1, and for the population difference between the J=0, M=0, and J=1, M=0, states, 1/T1=38.10±0.18 μsec−1⋅Torr−1. These results imply that not all collisions induce dipole‐allowed transitions. These values are consistent with previous linewidth values, beam maser experiments, and four‐level double resonance experiments.