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Six-loop renormalization group analysis of the $φ^4 + φ^6$ model

L. Ts. Adzhemyan, M. V. Kompaniets, A. V. Trenogin

TL;DR

The paper performs a six-loop renormalization-group analysis of the φ^4+φ^6 model in the ε-expansion about d = 3 − 2ε, focusing on tricritical behavior at the point where τ and λ vanish. By renormalizing in the G-scheme and computing the renormalization constants Z_i and RG functions up to six loops, the authors determine the fixed point u_* and tricritical exponents η, ν, ω, along with the parameter b_0 and the tricritical dimensions of composite operators Δ_{φ^k}. The results are compared to conformal-field-theory and non-perturbative RG predictions, showing full agreement with several classic works but revealing discrepancies with Hager02 due to typos, which the authors address in follow-up work. A Padé resummation to d = 2 provides approximate values for the exponents and composite dimensions, illustrating reasonable agreement with exact CFT values and non-perturbative RG results, and enabling a detailed cross-check of perturbative data against alternative frameworks.

Abstract

We investigate the $λ\ph^4+g\ph^6$ model using the renormalization group method and the $\ep$ expansion. This model is used in a situation where the coefficients $λ$, $g$ and the coefficient $τ$ of the term $τ\ph^2$ depend on two parameters $T$ and $P$, and there is a point ($T_c,P_c$) at which $τ$ and $λ$ are zero. This point is named the tricritical point. The description of a system depends on a trajectory that leads to the tricritical point on the plane ($T,P$). In the trajectories, when $λ$ goes to zero fast enough, the description is defined by the $\ph^6$ interaction and then the $\ph^4$ term can be considered as a composite operator. In this case, the logarithmic dimension is $d=3$, and the $\ep$ expansion is carried out in the dimension $d=3-2\ep$. The main exponents of the \textit{tricritical} model have been calculated in the third order of the $\ep$ expansion. Taking into account the $\ph^4$ interaction, we were able to calculate the value of the parameter that determines the required decrease rate in $λ$ to implement the tricritical behavior. The tricritical dimensions of the composite operators $\ph^k$ for $k=1, 2, 4, 6$ have been computed. The resulting values are compared to those known from a conformal field theory and non-perturbative renormalization group.

Six-loop renormalization group analysis of the $φ^4 + φ^6$ model

TL;DR

The paper performs a six-loop renormalization-group analysis of the φ^4+φ^6 model in the ε-expansion about d = 3 − 2ε, focusing on tricritical behavior at the point where τ and λ vanish. By renormalizing in the G-scheme and computing the renormalization constants Z_i and RG functions up to six loops, the authors determine the fixed point u_* and tricritical exponents η, ν, ω, along with the parameter b_0 and the tricritical dimensions of composite operators Δ_{φ^k}. The results are compared to conformal-field-theory and non-perturbative RG predictions, showing full agreement with several classic works but revealing discrepancies with Hager02 due to typos, which the authors address in follow-up work. A Padé resummation to d = 2 provides approximate values for the exponents and composite dimensions, illustrating reasonable agreement with exact CFT values and non-perturbative RG results, and enabling a detailed cross-check of perturbative data against alternative frameworks.

Abstract

We investigate the model using the renormalization group method and the expansion. This model is used in a situation where the coefficients , and the coefficient of the term depend on two parameters and , and there is a point () at which and are zero. This point is named the tricritical point. The description of a system depends on a trajectory that leads to the tricritical point on the plane (). In the trajectories, when goes to zero fast enough, the description is defined by the interaction and then the term can be considered as a composite operator. In this case, the logarithmic dimension is , and the expansion is carried out in the dimension . The main exponents of the \textit{tricritical} model have been calculated in the third order of the expansion. Taking into account the interaction, we were able to calculate the value of the parameter that determines the required decrease rate in to implement the tricritical behavior. The tricritical dimensions of the composite operators for have been computed. The resulting values are compared to those known from a conformal field theory and non-perturbative renormalization group.
Paper Structure (10 sections, 31 equations, 3 tables)