Mixture model — where it appears
Named by 3 essays across one field — each of them below, with the objects they name alongside it.
A spread the projection does not hide
A single projected spin–orbit angle says little about the true one, because the star's tilt is unknown. A population of nearly aligned systems is different: for small tilts the projected angle is one component of a two-component vector, so the rms true obliquity is exactly √2 times the rms projected angle — no star's inclination needed.
A fraction read in each channel's own units
Hot Jupiters arrive by two routes, one that ends at twice the planet's Roche distance and one that ends where the disc stopped. Fitting the mixture in Roche distances alone, as the edge invites, gives a fraction that drifts by almost half if the planets weigh more than assumed. Each route has to be read in the units in which it does not move — and then the answer is limited not by how well the planets are measured but by how their radii have changed since they arrived.
A second peak the errors have to let through
Whether the densest small planets are a population of their own or the far edge of the ordinary one is not a question about any single planet. It is a question about the shape of a histogram seen through measurement errors as wide as the gap it is looking for, and the number of planets it needs rises fifteen-fold for every factor of three in lost precision — which puts the answer a few dozen planets beyond the samples that first suggested it.
Named alongside it
The objects these essays reach for when they reach for this one.
Hot jupiterMeasurement errorCore mass fractionDisc migrationGiant impactsHigh-eccentricity migrationLikelihood ratioPlanet compositionPlanet migrationPopulation inferenceProjected obliquityRadius inflation