The adiabatic dissociation dynamics of NH2D((A) over tilde) and ND2H((A) ov
er tilde) have been probed by time-resolved Fourier transform infrared emis
sion spectroscopy. A product-state spectral pattern recognition technique i
s employed to separate out the emission features arising from the different
photofragmentation channels following the simultaneous excitation of mixtu
res of the four parent molecules NH3, NH2D, ND2H, and ND3 at 193.3 nm. The
rotational energy partitioning about the primary a-axis of the fragments NH
2((A) over tilde ,v(2)' = 0) and ND2((A) over tilde ,v(2)' = 0) from NH2D(A
) and ND2H((A) over tilde), respectively, is bimodal. We suggest that the o
rigin of this excitation reflects the competition between two distinct diss
ociation mechanisms that sample two different geometries during the bond cl
eavage. A larger quantum yield for producing ND2((A) over tilde ,v(2)' = 0)
from the photodissociation of ND2H than ND3 is attributed to the lower dis
sociation energy of the N-H as compared with the N-D bond and to the enhanc
ed tunneling efficiency of H atoms over D atoms through the barrier to diss
ociation. Similarly, the quantum yield for producing the NH2((A) over tilde
,v(2)' = 0) fragment is lower when an N-D bond must be cleaved in comparis
on to an N-H bond. Photodissociation of ND2H by cleavage of an N-H bond lea
ds to an ND2((A) over tilde) fragment with a much larger degree of vibratio
nal excitation (v(2)' = 1,2), accompanied by substantial rotation about the
minor b/c-axes, than when an N-D bond is cleaved in the photodissociation
of ND3. The quantum yield for producing NHD((A) over tilde) is larger for c
leavage of an N-H bond from NH2D than by cleavage of an N-D from ND2H.