We show that the honeycomb tight-binding model hosts an exact microscopic avatar of its low-energy SU(2) valley symmetry and parity anomaly. Specifically, the SU(2) valley symmetry arises from a collection of conserved, integer-quantized charge operators that obey the Onsager algebra. Along with lattice reflection and time-reversal symmetries, this Onsager symmetry has a Lieb-Schultz-Mattis (LSM) anomaly that matches the parity anomaly in the IR. Indeed, we show that any local Hamiltonian commuting with these symmetries cannot have a trivial unique gapped ground state. We study the phase diagram of the simplest symmetric model and survey various deformations, including Haldane’s mass term, which preserves only the Onsager symmetry. Our results place the parity anomaly in $2+1\mathrm{D}$ alongside Schwinger’s anomaly in $1+1\mathrm{D}$ and Witten’s SU(2) anomaly in $3+1\mathrm{D}$ as ’t Hooft anomalies that can arise from the Onsager symmetry on the lattice.

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• Anomalies
• Majorana fermions
• Quantum field theory
• Honeycomb lattice
• T-symmetry