State-to-state relaxation rates have been determined for ozone in coll
isions with itself and with nitrogen by two different methods. A theor
etical model of collisional broadening of ozone lines, the quantum Fou
rier transform theory with improved dynamics, was adapted to compute s
tate-to-state inelastic contributions to the pressure-broadened halfwi
dths for ozone-nitrogen collisions. These quantities were then determi
ned experimentally using time-resolved infrared double resonance spect
roscopy and a kinetic model for relaxation. Comparisons of kinetic mod
el simulations and experimental double-resonance signals confirmed a p
ropensity for first-order dipolar transitions, but also clearly demons
trated the importance of higher-order interactions leading to large ch
anges in J in single collisions. Simple energy and angular-momentum-sc
aling laws were found to be inadequate to represent the experimental d
ata.