Abstract

The pseudofermion functional renormalization group (PFFRG) method has proven to be a powerful numerical approach to treat frustrated quantum spin systems. In its usual implementation, however, the complex fermionic representation of spin operators introduces unphysical Hilbert-space sectors which render an application at finite temperatures inaccurate. In this work we formulate a general functional renormalization group approach based on Majorana fermions to overcome these difficulties. We, particularly, implement spin operators via an $\text{SO}(3)$ symmetric Majorana representation which does not introduce any unphysical states and, hence, remains applicable to quantum spin models at finite temperatures. We apply this scheme, dubbed pseudo-Majorana functional renormalization group (PMFRG) method, to frustrated Heisenberg models on small spin clusters as well as square and triangular lattices. Computing the finite-temperature behavior of spin correlations and thermodynamic quantities such as free energy and heat capacity, we find good agreement with exact diagonalization and the high-temperature series expansion down to moderate temperatures. We observe a significantly enhanced accuracy of the PMFRG compared to the PFFRG at finite temperatures. More generally, we conclude that the development of functional renormalization group approaches with Majorana fermions considerably extends the scope of applicability of such methods.

Highlights

  • Finding numerical solutions of quantum many-body problems is one of the core disciplines in modern condensed matter theory

  • For T 0.2, we find a very close agreement between the susceptibility obtained via pseudo-Majorana functional renormalization group (PMFRG) and the exact result from Eq (64)

  • We show analogous results of the pseudofermion functional renormalization group (PFFRG), where the presence of unphysical states seriously compromises the accuracy of the results at any finite-temperature scale

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Summary

Introduction

Finding numerical solutions of quantum many-body problems is one of the core disciplines in modern condensed matter theory. In a wide range of physical settings the problem amounts to analyze ground-state and finite-temperature phases of a system of interacting spins on a lattice. Even though the corresponding microscopic models are often conceptually simple, such as two-body Heisenberg spin Hamiltonians, they may harbor a colorful range of physical phenomena including exotic types of long-range orders [1], quantum phase transitions [2,3], or quantum spin liquids [4,5,6]. While quantum spin phases are traditionally described in terms of broken or unbroken symmetries, a more modern understanding includes concepts such as long-range entanglement or topological order [7] and reaches out to applications in the context of quantum information processing [8].

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