The state-dependence of the climate sensitivity is of great interest when studying climate change as it influences the interpretation of the proxy record (Kutzbach et al., 2013;Manabe & Bryan, 1985), historical temperature observations (Andrews, 2014;Gregory & Andrews, 2016), and the interpretation of differences among models (Bourdin et al., 2021). Recent modeling studies, ranging from conceptual (Meraner et al., 2013) to cloud-resolving models (Romps, 2020), find that after an initial decrease the magnitude of the clear-sky feedback parameter, λ, again increases at yet higher surface temperatures (T s ). This non-monotonicity manifests itself as a pronounced "bump," a maximum in the clear-sky climate sensitivity, 𝐴𝐴 , at T s ≈ 310 K. Some studies (e.g., Popp et al., 2016;Schneider et al., 2019;Wolf & Toon, 2015) detect different cloud mechanisms that may cause a local maximum in climate sensitivity. In this study, however, we focus on the growing but still inconclusive literature on the seemingly simpler question of the clear-sky radiative response to warming.Seeley and Jeevanjee (2021) describe a physical mechanism that explains the changing temperature-dependence of λ: when the rise of the temperature is tied to the rise of CO 2 , the increased CO 2 concentration broadens the spectral interval over which CO 2 is the dominant absorber, thereby coupling the outgoing-longwave radiation (OLR) in these spectral regions to the tropospheric temperature, and hence T s in a way that leads to a more negative λ with warming. The work by Seeley and Jeevanjee (2021) provides an elegant physical explanation for the climate sensitivity "bump" in studies with varying CO 2 concentration