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Two Loop Scalar Self-Mass during Inflation

T. Brunier, V. K. Onemli, R. P. Woodard

TL;DR

The paper performs a complete two-loop computation of the fully renormalized scalar self-mass-squared for a massless, minimally coupled $\varphi^4$ field during inflation in a locally de Sitter background, employing the Schwinger-Keldysh formalism and dimensional regularization. It shows that curvature induces a nonzero mass renormalization and a time-dependent finite piece at one loop, and reveals a rich, causal nonlocal structure at two loops with overlapping divergences canceled by counterterms $\delta m^2$, $\delta \lambda$, and $\delta Z$; the final two-loop self-mass-squared comprises nonlocal derivative kernels and a local $a^4\delta^D(x-x')$ part with $\ln(a)$-dependent contributions. The work analyzes stability and links to stochastic inflation, suggesting possible initial-state modifications to account for exponentially decaying terms, and sets the stage for applying these results to the quantum-corrected field equations governing inflationary dynamics. Overall, the results demonstrate how inflationary expansion generates and regulates quantum corrections to scalar dynamics in a cosmological setting, with implications for early-universe phenomenology and stochastic approaches.

Abstract

We work in the locally de Sitter background of an inflating universe and consider a massless, minimally coupled scalar with a quartic self-interaction. We use dimensional regularization to compute the fully renormalized scalar self-mass-squared at one and two loop order for a state which is released in Bunch-Davies vacuum at t=0. Although the field strength and coupling constant renormalizations are identical to those of lfat space, the geometry induces a non-zero mass renormalization. The finite part also shows a sort of growing mass that competes with the classical force in eventually turning off this system's super-acceleration.

Two Loop Scalar Self-Mass during Inflation

TL;DR

The paper performs a complete two-loop computation of the fully renormalized scalar self-mass-squared for a massless, minimally coupled field during inflation in a locally de Sitter background, employing the Schwinger-Keldysh formalism and dimensional regularization. It shows that curvature induces a nonzero mass renormalization and a time-dependent finite piece at one loop, and reveals a rich, causal nonlocal structure at two loops with overlapping divergences canceled by counterterms , , and ; the final two-loop self-mass-squared comprises nonlocal derivative kernels and a local part with -dependent contributions. The work analyzes stability and links to stochastic inflation, suggesting possible initial-state modifications to account for exponentially decaying terms, and sets the stage for applying these results to the quantum-corrected field equations governing inflationary dynamics. Overall, the results demonstrate how inflationary expansion generates and regulates quantum corrections to scalar dynamics in a cosmological setting, with implications for early-universe phenomenology and stochastic approaches.

Abstract

We work in the locally de Sitter background of an inflating universe and consider a massless, minimally coupled scalar with a quartic self-interaction. We use dimensional regularization to compute the fully renormalized scalar self-mass-squared at one and two loop order for a state which is released in Bunch-Davies vacuum at t=0. Although the field strength and coupling constant renormalizations are identical to those of lfat space, the geometry induces a non-zero mass renormalization. The finite part also shows a sort of growing mass that competes with the classical force in eventually turning off this system's super-acceleration.

Paper Structure

This paper contains 13 sections, 103 equations, 5 figures.

Figures (5)

  • Figure 1: Generic one loop self-mass-squared.
  • Figure 2: Generic tree and one loop vertex function.
  • Figure 3: Generic Sunset Diagram.
  • Figure 4: Generic Snowman Diagram with mass counterterm.
  • Figure 5: Generic Counter Diagrams. The one on the left is the same as Fig. \ref{['fig1']} but with $\delta \lambda$ in place of $\lambda$. The one on the right is the field strength renormalization.