Significant populations of NO in excited vibrational levels
v ![[gt-or-equal]](https://www.rsc.org/images/entities/char_2a7e.gif)
2 have recently been observed in the lower thermosphere, for which the relaxation rates and pathways are largely governed by collisions with O atoms. Laboratory experiments can provide accurate kinetic parameters for modelling and interpreting such steady-state
v-dependent population distributions. In this study, a two-laser, pump–probe arrangement has been used to measure the fractional population of NO(
v − 1) arising from the collision-induced relaxation of NO(
v = 3) by O atoms and, in an ancillary experiment, NO(
v = 2, 3) by NO. The branching fraction
χ
O
(
v = 3→2) = 0.35 ± 0.12 for O-atom collisions. The
χ
O
value is consistent with a long-lived NO
2
*
collision complex, in which the total energy is randomly distributed among the internal degrees of freedom prior to dissociation, and agrees with a recent quasiclassical trajectory calculation. For collisions with NO,
χ
NO
(
v = 3→2) = 0.73 ± 0.19, indicating a significant multiquantum component. The branching fraction
χ
NO
(
v = 2→1) = 1.19 ± 0.31 can be considered an effective value only, since its interpretation relies on an assumption regarding the relaxation mechanism. The rate constants
k
O
(
v = 3) = (3.0 ± 0.6) × 10
−11
cm
3
s
−1
for the vibrational relaxation of NO(
v = 3) by O atoms, and
k
NO
(
v = 2) = (2.7 ± 0.5) × 10
−12
cm
3
s
−1
and
k
NO
(
v = 3) = (3.4 ± 0.7) × 10
−12
cm
3
s
−1
for the relaxation of NO(
v = 2, 3) by NO have also been obtained, and are in good agreement with previous results from this laboratory.