# Renormalization Scheme Dependence, RG Flow and Borel Summability in $\phi^4$ Theories in $d<4$

## TL;DR

This paper investigates how renormalization scheme choices affect the analysis of $^4$ theories below four dimensions, demonstrating that physical observables like the mass gap can confirm fixed points independently of RG scheme dependencies.

## Contribution

It introduces a family of renormalization schemes ensuring Borel summability and refines critical exponent calculations by extending perturbation theory orders.

## Key findings

- Borel summability depends on the renormalization scheme used.
- Physical observables can confirm fixed points without RG scheme dependence.
- Extended perturbation theory improves critical exponent estimates.

## Abstract

Renormalization group (RG) and resummation techniques have been used in $N$-component $\phi^4$ theories at fixed dimensions below four to determine the presence of non-trivial IR fixed points and to compute the associated critical properties. Since the coupling constant is relevant in $d<4$ dimensions, the RG is entirely governed by renormalization scheme-dependent terms. We show that the known proofs of the Borel summability of observables depend on the renormalization scheme and apply only in "minimal" ones, equivalent in $d=2$ to an operatorial normal ordering prescription, where the $\beta$-function is trivial to all orders in perturbation theory. The presence of a non-trivial fixed point can be unambiguously established by considering a physical observable, like the mass gap, with no need of RG techniques. Focusing on the $N=1$, $d=2$ $\phi^4$ theory, we define a one-parameter family of renormalization schemes where Borel summability is guaranteed and study the accuracy on the determination of the critical exponent $\nu$ as the scheme is varied. While the critical coupling shows a significant sensitivity on the scheme, the accuracy in $\nu$ is essentially constant. As by-product of our analysis, we improve the determination of $\nu$ obtained with RG methods by computing three more orders in perturbation theory.