Theory of criticality-enabled $U(1)$ symmetry breaking in a class of 1+1D systems

Abstract

We develop an analytic theory of the recently proposed $U(1)$ symmetry breaking at interacting 1+1D Lifshitz quantum critical points. The low-energy theory contains two compact fields, $\theta$ and $\varphi$, coupled by a Berry term that makes $\theta$ canonically conjugate to the conserved density ${\partial }_x\varphi$. Within a controlled large-$N$ limit, we establish long-range order (LRO) of $e^{i\beta \theta }$ and stretched-exponential decay of the conjugate vertex, $\log ⟨e^{i\beta \varphi (x)}{e}^{-i\beta \varphi (0)}⟩\propto -|\beta {|}^{4/3}|x{|}^{2/3}$. Beyond large $N$, we argue that $U(1)$ LRO follows if the dynamical exponent satisfies $z\ne 1$, consistent with existing calculations. Using finite-size and infinite-system DMRG, we study an itinerant-electron chain with $U(1)⋊{\mathbb{Z}}_2$ symmetry, whose spin sector realizes this theory at a ferromagnetic quantum critical point. We find spin-nematic LRO in $S_i^{+}{S}_{i+1}^{+}$ and stretched-exponential electron Green's functions, revealing distinctive non-Gaussian signatures of criticality-enabled order.