Slow-roll curvature power spectrum
= Slow-roll curvature power spectrum
{title2=$\Delta_{\mathcal R}^2$}
At leading order in canonical single-field slow roll and evaluated at horizon exit $k=aH$,
$$
\Delta_{\mathcal R}^2(k)=\frac1{2\epsilon M_{\rm Pl}^2}
\left(\frac{H}{2\pi}\right)^2.
$$