Heat redistribution — where it appears
Named by 2 essays across one field — each of them below, with the objects they name alongside it.
The planet is seen when it disappears
Half an orbit after the transit the planet passes behind its star, and the light that vanishes is the planet's own. Subtracting two brightnesses taken hours apart isolates a body nothing has ever resolved.
A day side as hot as bare rock
A planet with no air can be no hotter on its day side than bare rock that re-radiates every photon where it lands. An atmosphere carries some of that heat to the night side, so the day side comes out cooler. For a rocky planet too small for its spectrum to be read, that difference is the test: three of the first four small planets around red dwarfs measured this way sit at the bare-rock limit, and the fourth sits below it by an amount that a thin atmosphere, or a brighter surface, could explain equally well.
Named alongside it
The objects these essays reach for when they reach for this one.
Phase curveSecondary eclipseTidal lockingAlbedoAtmospheric escapeBond albedoBrightness temperatureDay night contrastEmission spectrumHot spot offsetM dwarfOccultation