We study renormalization group multicritical fixed points in the ϵ-expansion of scalar field theories characterized by the symmetry of the (hyper)cubic point group HN. After reviewing the algebra of HN-invariant polynomials and arguing that there can be an entire family of multicritical (hyper)cubic solutions with ϕ2n interactions in d=2nn−1−ϵ dimensions, we use the general multicomponent beta functionals formalism to study the special cases d = 3 − ϵ and d=83−ϵ, deriving explicitly the beta functions describing the flow of three- and four-critical (hyper)cubic models. We perform a study of their fixed points, critical exponents and quadratic deformations for various values of N, including the limit N = 0, that was reported in another paper in relation to the randomly diluted single-spin models, and an analysis of the large N limit, which turns out to be particularly interesting since it depends on the specific multicriticality. We see that, in general, the continuation in N of the random solutions is different from the continuation coming from large-N, and only the latter interpolates with the physically interesting cases of low-N such as N = 3. Finally, we also include an analysis of a theory with quintic interactions in d=103−ϵ and, for completeness, the NNLO computations in d = 4 − ϵ.

Multicritical hypercubic models

Zanusso O.
2021-01-01

Abstract

We study renormalization group multicritical fixed points in the ϵ-expansion of scalar field theories characterized by the symmetry of the (hyper)cubic point group HN. After reviewing the algebra of HN-invariant polynomials and arguing that there can be an entire family of multicritical (hyper)cubic solutions with ϕ2n interactions in d=2nn−1−ϵ dimensions, we use the general multicomponent beta functionals formalism to study the special cases d = 3 − ϵ and d=83−ϵ, deriving explicitly the beta functions describing the flow of three- and four-critical (hyper)cubic models. We perform a study of their fixed points, critical exponents and quadratic deformations for various values of N, including the limit N = 0, that was reported in another paper in relation to the randomly diluted single-spin models, and an analysis of the large N limit, which turns out to be particularly interesting since it depends on the specific multicriticality. We see that, in general, the continuation in N of the random solutions is different from the continuation coming from large-N, and only the latter interpolates with the physically interesting cases of low-N such as N = 3. Finally, we also include an analysis of a theory with quintic interactions in d=103−ϵ and, for completeness, the NNLO computations in d = 4 − ϵ.
2021
Zinati, R. B. A.; Codello, A.; Zanusso, O.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11568/1121007
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