Abstract

Magnetic fluctuations and electrons couple in intriguing ways in the vicinity of zero temperature phase transitions - quantum critical points - in conducting materials. Quantum criticality is implicated in non-Fermi liquid behavior of diverse materials, and in the formation of unconventional superconductors. Here we uncover an entirely new type of quantum critical point describing the onset of antiferromagnetism in a nodal semimetal engendered by the combination of strong spin-orbit coupling and electron correlations, and which is predicted to occur in the iridium oxide pyrochlores. We formulate and solve a field theory for this quantum critical point by renormalization group techniques, show that electrons and antiferromagnetic fluctuations are strongly coupled, and that both these excitations are modified in an essential way. This quantum critical point has many novel features, including strong emergent spatial anisotropy, a vital role for Coulomb interactions, and highly unconventional critical exponents. Our theory motivates and informs experiments on pyrochlore iridates, and constitutes a singular realistic example of a non-trivial quantum critical point with gapless fermions in three dimensions.

Highlights

  • Antiferromagnetic quantum critical points (QCPs) are controlled by the interactions between electrons and magnetic fluctuations [1,2]

  • The electronic Fermi surface and order parameter are strongly coupled, a fact which may be related to high-temperature superconductivity and associated phenomena

  • We consider a quadratic band touching at the Fermi energy, as in the inverted band-gap material HgTe, but having in mind the strongly correlated family of iridium oxide pyrochlores [9,10,11,12]

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Summary

INTRODUCTION

Antiferromagnetic quantum critical points (QCPs) are controlled by the interactions between electrons and magnetic fluctuations [1,2]. We show that the replacement of the Fermi surface by a point Fermi node alters the physics in an essential way, suppressing screening of the Coulomb interaction and allowing the order-parameter fluctuations to affect all the low-energy electrons These two facts lead to a strongly-coupled quantum critical point. The nodal nature of the Fermi point, happily, enables a rather complete analysis of the problem, which we present here, using the powerful renormalization group (RG) technique This is because both the collective orderparameter fluctuations and the low-energy quasiparticles have their excitation minima at a single point in momentum space (here at k 1⁄4 0), unlike the case of criticality in a metal, where the electronic quasiparticles have their minima at an extended Fermi surface.

All-in-all-out order
Electronic structure and phases
RENORMALIZATION GROUP
Extreme anisotropy limit
Fermion self-energy and vertex corrections
Scaling properties
Logarithmic corrections and extreme anisotropy
Comparison to Hertz-Millis and mean-field theories
Beyond large N
Experiments
Couplings
Green’s function and self-energy conventions
Coefficient of the logarithm
Approximation
Diagram expressions
Flow equations
Details of the flows of c1 and c2
Exponents
Solutions to the flow equations
Order-parameter exponent
Specific heat
Full Text
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