Cosmological entropy perturbation Created 2026-09-28 Updated 2026-11-05
A cosmological entropy perturbation describes relative composition changes between cosmic components, rather than only a common displacement along the background evolution. For cold dark matter and photons, define fractional density perturbations and . Their relative entropy variable is
The factor follows from the different background dilution laws and , with scale factor . Under a first-order time shift , the density perturbation gauge transformation gives and , where . These shifts cancel in .
Thus this relative entropy is gauge invariant at first order. The condition gives the common adiabatic relation . A pure isocurvature perturbation initial condition is chosen with vanishing initial comoving curvature perturbation; a mixed initial state can instead have both nonzero curvature and nonzero . Vanishing initial curvature is therefore a condition on a pure initial mode, not a requirement for defining the relative entropy variable.
The supplied superhorizon evolution equation is
For an adiabatic cosmological perturbation, , so and the comoving curvature perturbation is conserved on superhorizon scales.
For photons and cold dark matter, put , , and use , , and . Then
The cosmological entropy perturbation implies , so the adiabatic part cancels and
Since , the curvature evolves as
In the sign convention requested in the question, , this means