  Reheating is a transition era after the end of inflation, during which the
inflaton is converted into the particles that populate the Universe at later
times. No direct cosmological observables are normally traceable to this period
of reheating. Indirect bounds can however be derived. One possibility is to
consider cosmological evolution for observable CMB scales from the time of
Hubble crossing to the present time. Depending upon the model, the duration and
final temperature after reheating, as well as its equation of state, may be
directly linked to inflationary observables. For single-field inflationary
models, if we approximate reheating by a constant equation of state, one can
derive relations between the reheating duration (or final temperature), its
equation of state parameter, and the scalar power spectrum amplitude and
spectral index. While this is a simple approximation, by restricting the
equation of state to lie within a broad physically allowed range, one can in
turn bracket an allowed range of $n_s$ and $r$ for these models. The added
constraints can help break degeneracies between inflation models that otherwise
overlap in their predictions for $n_s$ and $r$.
