Abstract

The field-theoretical model describing multicritical phenomena with two coupled order parameters with n_{||} and n_{\perp} components and of O(n_{||}) \oplus O(n_{\perp}) symmetry is considered. Conditions for realization of different types of multicritical behaviour are studied within the field-theoretical renormalization group approach. Surfaces separating stability regions for certain types of multicritical behaviour in parametric space of order parameter dimensions and space dimension d are calculated using the two-loop renormalization group functions. Series for the order parameter marginal dimensions that control the crossover between different universality classes are extracted up to the fourth order in \varepsilon=4-d and to the fifth order in a pseudo-\varepsilon parameter using the known high-order perturbative expansions for isotropic and cubic models. Special attention is paid to a particular case of O(1) \oplus O(2) symmetric model relevant for description of anisotropic antiferromagnets in an external magnetic field.

Highlights

  • The concept of universality plays a paradigmatic role in the modern statistical physics

  • In the n–d-space, the regions of stable fixed point (FP) are separated by borders and the n(d) curves define the order parameter (OP) marginal dimensions that control the crossover between different universality classes

  • In the present paper we have studied the conditions under which different types of multicritical behaviour are realized for the O(n ) ⊕ O(n⊥) model

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Summary

Introduction

The concept of universality plays a paradigmatic role in the modern statistical physics. Conditions for realization of different types of multicritical behaviour, that are defined by the relation between the dimensions of the OPs n , n⊥, were obtained already in the first nontrivial approximation of the field-theoretical RG for d < 4 [8, 17, 18]. They determine the stability regions in the parametric.

The model and RG picture of its multicritical phenomena
Stability border-surfaces within a two-loop order approximation
BSs from ε-expansion
BSs from resummed β-functions
High loop order results for marginal dimensions
Five-loop ε-expansions for marginal dimensions
Conclusion
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