mFor formaldehyde, the C -0 stretch potential of '(T, r*) crosses all 'A, Rydberg \r, r* + 2 system to these Rydberg states. For thioformaldehyde, the situation is similar but a shift in the potentials allows for direct observation of '(r, T * ) . In its ' ( T , T * ) state, H,CO is planar, having a low barrier of about 0.2 eV toward the nonplanar '(v, T * > state. For H,CS, the planar conformation of ' ( T , r*) is a saddle point, with '(v, r*) being the global minimum on the 2'A' surface. The triplet r, r* states of H,CO and H,CS are nonplanar, having inversion barriers of 0.1 and 0.05 eV, respectively. For both H,CO and H,CS, the T , r* configuration also crosses the ground-state configuration, which explains predissociation and radiationless transitions of some Rydberg states.otentials, such as n, 3p,, n, 3d,,, etc., thereby transferring the intensity of the unassigned 0 1996 John Wiley & Sons, Inc.