At exoplanet secondary eclipse, the full-phase planet-star flux ratio is the sum of reflected and thermal light. Approximating both bodies as unresolved blackbodies and taking wavelength-independent geometric albedo,
The first term is a flat reflected-light level under the stated constant-albedo assumption. At short wavelength the cool planet lies in the Wien limit, so thermal emission is exponentially suppressed and reflection dominates. At long wavelength both spectra enter the Rayleigh-Jeans law, giving
The sketch therefore starts on the reflected plateau, rises where planetary blackbody radiation becomes important, and asymptotically approaches the long-wavelength plateau. This neglects spectral albedo features, phase dependence, stellar lines, and a nonisothermal planetary photosphere.
Figure 1.
Schematic wavelength dependence of a planet-star flux ratio at secondary eclipse
. Reflected light sets a short-wavelength plateau, planetary blackbody emission produces a thermal rise, and the sum approaches its Rayleigh--Jeans plateau at long wavelength. The temperatures and radii are illustrative rather than a fit to a particular planet. Details.

Articles by others on the same topic (0)

There are currently no matching articles.