- Open Access
Emergent Spacetime Supersymmetry at 2D Fractionalized Quantum Criticality
Phys. Rev. Lett. 136, 256502 – Published 24 June, 2026
DOI: https://doi.org/10.1103/zqnh-tb1d
Abstract
While experimental evidence for spacetime supersymmetry (SUSY) in particle physics remains elusive, condensed matter systems offer a promising arena for its emergence at quantum critical points (QCPs). Although there have been a variety of proposals for emergent SUSY at symmetry-breaking QCPs, the emergence of SUSY at fractionalized QCPs remains largely unexplored. Here, we demonstrate emergent spacetime SUSY at a fractionalized QCP in the Kitaev honeycomb model with Su-Schrieffer-Heeger (SSH) spin-phonon coupling. Specifically, through numerical computations and analytical analysis, we show that the anisotropic SSH-Kitaev model hosts a fractionalized QCP between a Dirac spin liquid and an incommensurate or commensurate valence-bond-solid phase coexisting with topological order. A low-energy field theory incorporating phonon quantum fluctuations reveals that this fractionalized QCP features an emergent spacetime SUSY. We further discuss their universal experimental signatures in thermal transport and viscosity, highlighting the concrete lattice realization of emergent SUSY at a fractionalized QCP in 2D.
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Strictly speaking, the physical state is an equal weight superposition of all the states connected to the gauge-fixed wave function by gauge transformations [45]. Nevertheless, the behavior of physical–gauge-invariant quantities, such as emergent SUSY or correlation functions, are the same as those obtained in the field theory developed below by fixing the gauge.
Here, does not mean the corner of the Brillouin zone, since we have included anisotropic hoppings of the Majorana fermions.
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