Short-period gas giants (hot Jupiters) on circular orbits are expected to be tidally locked into synchronous rotation, with permanent daysides that face their host stars, and permanent nightsides that face the darkness of space 1 . Thermal flux from the nightside of several hot Jupiters has been measured, meaning energy is transported from day to night in some fashion. However, it is not clear exactly what the physical information from these detections reveals about the atmospheric dynamics of hot Jupiters. Here we show that the nightside effective temperatures of a sample of 12 hot Jupiters are clustered around 1100 K, with a slight upward trend as a function of stellar irradiation. The clustering is not predicted by cloud-free atmospheric circulation models 2-4 . This result can be explained if most hot Jupiters have nightside clouds that are optically thick to outgoing longwave radiation and hence radiate at the cloud-top temperature, and progressively disperse for planets receiving greater incident flux. Phase curve observations at a greater range of wavelengths are crucial to determining the extent of cloud coverage, as well as the cloud composition on hot Jupiter nightsides 5, 6 .We collected published full orbit, infrared phase curves for twelve hot Jupiters: CoRoT-2b 7 , HAT-P-7-b 8 , HD 149026b 9 , HD 189733b 10 , HD 209458b 11 , WASP-12b 12 , WASP-14b 13 , WASP-18b 14 , WASP-19b 8 , WASP-33b 9 , WASP-43b [15][16][17][18] . We also included the brown dwarf KELT-1b 20 . We calculated the nightside brightness temperatures from the phase curve parameters, and used Gaussian Process regression to estimate each planet's bolometric flux, and subsequently its disk-integrated nightside effective temperature. Several of the published phase curve fits imply negative nightside disk-integrated flux, which is unphysical, because it implies that the planets have negative brightness at some longitudes on their surface. We explain how we handled these cases in the Methods section. Future phase curve observations should be fit with the constraint that flux is non-negative everywhere on the planet. We also inferred nightside temperatures by considering and modifying negative brightness maps, which is similar in spirit to demanding positive phase curves and brightness maps when fitting the data. The mapping approach 1 arXiv:1809.00002v2 [astro-ph.EP] 23 Aug 2019 yielded a nightside temperature trend consistent with that of the disk-integrated approach.In Figure 1 we show the dayside and nightside effective temperatures plotted against the stellar irradiation temperature, T 0 ≡ T R /a, were T is the stellar effective temperature, R is the stellar radius, and a is semi-major axis. The nightside temperatures are all around 1100K and exhibit a slight upward trend with stellar irradiation. We tabulate the dayside temperature, nightside temperature, Bond Albedo, and heat recirculation efficiency for each planet in Table 1.Various theories have suggested that reradiation 1 , advection, wave propagation 21 , molecular dissocation 2...