C-P-T anomaly matching in bosonic quantum field theory and spin chains

TL;DR

This paper investigates a mixed 't Hooft anomaly involving charge conjugation, parity, and time-reversal symmetries in 1+1D bosonic quantum field theories, revealing constraints on the ground state and connecting field theory anomalies to spin chain properties.

Contribution

It identifies a novel $C$-$P$-$T$ anomaly in the $O(3)$ nonlinear sigma model and spin chains, and explores its implications for ground state gappability and symmetry constraints.

Findings

Anomaly exists at $ heta= ext{pi}$ in the $O(3)$ model.

Ground state cannot be trivially gapped if $C$, $P$, and $T$ are preserved.

Anomaly extends to $ ext{C}P^{N-1}$ models for even $N$.

Abstract

We consider the $O(3)$ nonlinear sigma model with the $\theta$-term and its linear counterpart in 1+1D. The model has discrete time-reflection and space-reflection symmetries at any $\theta$, and enjoys the periodicity in $\theta\rightarrow \theta+2\pi$. At $\theta=0,\pi$ it also has a charge-conjugation $C$-symmetry. Gauging the discrete space-time reflection symmetries is interpreted as putting the theory on the nonorientable $\mathbb RP^2$ manifold, after which the $2\pi$ periodicity of $\theta$ and the $C$ symmetry at $\theta=\pi$ are lost. We interpret this observation as a mixed 't Hooft anomaly among charge-conjugation $C$, parity $P$, and time-reversal $T$ symmetries when $\theta=\pi$. Anomaly matching implies that in this case the ground state cannot be trivially gapped, as long as $C$, $P$ and $T$ are all good symmetries of the theory. We make several consistency checks with various semi-classical regimes, and with the exactly solvable XYZ model. We interpret this anomaly as an anomaly of the corresponding spin-half chains with translational symmetry, parity and time reversal (but not involving the $SO(3)$-spin symmetry), requiring that the ground state is never trivially gapped, even if $SO(3)$ spin symmetry is explicitly and completely broken. We also consider generalizations to $\mathbb{C}P^{N-1}$ models and show that the $C$-$P$-$T$ anomaly exists for even $N$.