Beyond self-healing: Stabilizing and destabilizing photochemical adjustment of the ozone layer

Published in Atmospheric Chemisty and Physics, 2024

Match, A., E. P. Gerber, and S. Fueglistaler, 2024: Beyond self-healing: Stabilizing and destabilizing photochemical adjustment of the ozone layer, Atmos. Chem. Phys., 24, 10305-10322, https://doi.org/10.5194/acp-24-10305-2024.

Official Version.

The ozone layer is often noted to exhibit self-healing, whereby depletion of ozone aloft induces ozone increases below, explained to result from enhanced ozone production due to the associated increase in UV radiation below. Similarly, ozone enhancement aloft can reduce ozone below (reverse self-healing). This paper considers self-healing and reverse self-healing to manifest a general mechanism we call photochemical adjustment, whereby ozone perturbations lead to a downward cascade of anomalies in UV and ozone. Conventional explanations for self-healing imply that photochemical adjustment is stabilizing, damping perturbations towards the surface. However, photochemical adjustment can be destabilizing if the enhanced UV disproportionately increases the ozone sink, as can occur if that UV photolyzes ozone to produce atomic oxygen that speeds up catalytic destruction of ozone. We analyze photochemical adjustment in two linear ozone models (Cariolle v2.9 and LINOZ), finding that: (1) photochemical adjustment is destabilizing above 40 km in the tropical stratosphere, and (2) self-healing often represents only a small fraction of the total photochemical stabilization. The destabilizing regime above 40 km is reproduced in a much simpler model: the Chapman Cycle augmented with destruction of O and O3 by generalized catalytic cycles and transport (the Chapman+2 model). The Chapman+2 model reveals that photochemical destabilization occurs where the ozone sink is more sensitive than the source to perturbations in overhead column ozone, which is found to occur if the window of overlapping absorption by O2 and O3 is optically unsaturated, i.e., where overhead slant column ozone is below approximately 10^18 molec cm^−2