Quantum radiative corrections to slow-roll inflation
Ante Bilandzic, Tomislav Prokopec
TL;DR
The paper develops a renormalization-group improved one-loop framework to calculate quantum radiative corrections to slow-roll inflation in a nonminimally coupled ${\lambda}\varphi^4$ model in de Sitter space. By combining the Chernikov-Tagirov propagator with RG-improved effective potentials, it derives quantum corrections to the slow-roll parameters $\epsilon$ and $\eta$, the scalar spectral index $n_s$, the tensor spectral index $n_g$, and the tensor-to-scalar ratio $r$, showing an infrared enhancement that scales with the number of e-foldings $N$. The leading quantum contributions are suppressed by the small coupling $\lambda$ (as $\lambda N^2$ or $\lambda N$ depending on the observable), leading to unobservable corrections for realistic parameter values ($\lambda \sim 10^{-12}$, $N\sim 50$–60), though the framework provides explicit, RG-consistent expressions for these corrections. The work highlights the role of curvature couplings and infrared effects in curved-space inflation and outlines avenues to extend the analysis to quasi-de Sitter backgrounds and other matter sectors.
Abstract
We consider the nonminimally coupled lambda phi^4 scalar field theory in de Sitter space and construct the renormalization group improved renormalized effective theory at the one-loop level. Based on the corresponding quantum Friedmann equation and the scalar field equation of motion, we calculate the quantum radiative corrections to the scalar spectral index n_s, gravitational wave spectral index n_g and the ratio r of tensor to scalar perturbations. When compared with the standard (tree-level) values, we find that the quantum contributions are suppressed by lambda N^2 where N denotes the number of e-foldings. Hence there is an N^2 enhancement with respect to the naive expectation, which is due to the infrared enhancement of scalar vacuum fluctuations characterising de Sitter space. Since observations constrain lambda to be very small lambda ~ 10^(-12) and N ~ 50-60, the quantum corrections in this inflationary model are unobservably small.
