Reexamination of the nonperturbative renormalization-group approach to the Kosterlitz-Thouless transition

TL;DR

This paper reexamines the Kosterlitz-Thouless transition using a nonperturbative renormalization-group approach, confirming key universal features and providing results consistent with exact values.

Contribution

It demonstrates that the nonperturbative renormalization-group method can accurately reproduce the universal properties of the KT transition.

Findings

Reproduces the anomalous dimension η ≈ 0.24 at T_KT

Finds the stiffness jump ρ_s ≈ 0.64 at T_KT

Confirms the essential singularity of correlation length as T approaches T_KT

Abstract

We reexamine the two-dimensional linear O(2) model ($\varphi^4$ theory) in the framework of the nonperturbative renormalization-group. From the flow equations obtained in the derivative expansion to second order and with optimization of the infrared regulator, we find a transition between a high-temperature (disordered) phase and a low-temperature phase displaying a line of fixed points and algebraic order. We obtain a picture in agreement with the standard theory of the Kosterlitz-Thouless (KT) transition and reproduce the universal features of the transition. In particular, we find the anomalous dimension $\eta(\Tkt)\simeq 0.24$ and the stiffness jump $\rho_s(\Tkt^-)\simeq 0.64$ at the transition temperature $\Tkt$, in very good agreement with the exact results $\eta(\Tkt)=1/4$ and $\rho_s(\Tkt^-)=2/\pi$, as well as an essential singularity of the correlation length in the high-temperature phase as $T\to \Tkt$.