Anomalous dimensions of monopole operators at the transitions between Dirac and topological spin liquids
\'Eric Dupuis, Rufus Boyack, William Witczak-Krempa

TL;DR
This paper calculates the anomalous dimensions of monopole operators at quantum critical points between Dirac and topological spin liquids using conformal field theory, revealing near-equal scaling dimensions with distinct quantum fluctuation origins.
Contribution
It provides the first sub-leading order monopole scaling dimensions for various QSL transitions, compares them across models, and verifies universal asymptotic behavior in large charge limits.
Findings
Monopole scaling dimension for minimal charge q=1/2 is approximately 2N*0.26510 with quantum corrections.
Quantum fluctuations differ in origin despite similar scaling dimensions for different spin liquids.
Large-q asymptotics match universal non-perturbative predictions for conformal field theories.
Abstract
Monopole operators are studied in a large family of quantum critical points between Dirac and topological quantum spin liquids (QSLs): chiral and Z QSLs. These quantum phase transitions are described by conformal field theories (CFTs): quantum electrodynamics in 2+1 dimensions with 2N flavors of two-component massless Dirac fermions and a four-fermion interaction. For the transition to a chiral spin liquid, it is the Gross-Neveu interaction (QED-GN), while for the transitions to Z QSLs it is a superconducting pairing term with general spin/valley structure (generalized QED-ZGN). Using the state-operator correspondence, we obtain monopole scaling dimensions to sub-leading order in 1/N. For monopoles with a minimal topological charge q=1/2, the scaling dimension is 2N*0.26510 at leading-order, with the quantum correction being 0.118911(7) for the chiral spin…
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Taxonomy
TopicsTopological Materials and Phenomena · Advanced Condensed Matter Physics · Quantum many-body systems
