Abstract

We demonstrate that there does exist an equilibrium description of thermodynamics on the apparent horizon in the expanding cosmological background for a wide class of modified gravity theories with the Lagrangian density f(R,ϕ,X)f(R, ϕ, X), where RR is the Ricci scalar and XX is the kinetic energy of a scalar field ϕϕ. This comes from a suitable definition of an energy momentum tensor of the "dark" component obeying the local energy conservation law in the Jordan frame. It is shown that the equilibrium description in terms of the horizon entropy SS is convenient because it takes into account the contribution of the horizon entropy S^\hat{S} in non-equilibrium thermodynamics as well as an entropy production term.

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