Aerosol-cloud interactions, especially for ice and mixed-phase clouds, are a major source of uncertainty for predicting weather and climate change (Bellouin et al., 2020;Forbes & Ahlgrimm, 2014;McCoy et al., 2016). On average, clouds cool the planet; however, the cloud radiative effect (CRE) depends strongly on the number and size of hydrometeors (Seinfeld et al., 2016). Particularly, cloud optical thickness is tied to the hydrometeor surface area. Thus, a cloud with a large number of small hydrometeors will be more reflective compared to a cloud of the same condensed water content composed of a small number of large hydrometeors (Twomey, 1974). Moreover, a cloud composed of larger hydrometeors will be shorter lived: the larger hydrometeors will precipitate faster out of the atmosphere (Albrecht, 1989).Ice-nucleating particles (INPs) can trigger droplet freezing between 0°C and −35°C (Hoose & Möhler, 2012); subsequently, ice particles grow at the expense of depleting liquid cloud droplets (Bergeron, 1935;Findeisen et al., 2015;Wegener, 1911). The number of ice particles is typically orders of magnitude smaller compared to the number of cloud droplets and their size is several times larger than the typical cloud droplet size. Therefore, at temperatures warmer than −35°C, INP-driven droplet freezing is associated with less reflecting clouds and a warming effect on climate (