Quantum scars from zero modes in an Abelian lattice gauge theory on ladders

Abstract

We consider the spectrum of a $U(1)$ quantum link model where gauge fields are realized as $S=1/2$ spins and demonstrate a new mechanism for generating quantum many-body scars (high-energy eigenstates that violate the eigenstate thermalization hypothesis) in a constrained Hilbert space. Many-body dynamics with local constraints has attracted much attention due to the recent discovery of non-ergodic behavior in quantum simulators based on Rydberg atoms. Lattice gauge theories provide natural examples of constrained systems since physical states must be gauge-invariant. In our case, the Hamiltonian $H={\mathcal{O}}_{\mathrm{kin}}+\lambda {\mathcal{O}}_{\mathrm{pot}}$, where ${\mathcal{O}}_{\mathrm{pot}}$ (${\mathcal{O}}_{\mathrm{kin}}$) is diagonal (off-diagonal) in the electric flux basis, contains exact mid-spectrum zero modes at $\lambda =0$ whose number grows exponentially with system size. This massive degeneracy is lifted at any non-zero $\lambda$ but some special linear combinations that simultaneously diagonalize ${\mathcal{O}}_{\mathrm{kin}}$ and ${\mathcal{O}}_{\mathrm{pot}}$ survive as quantum many-body scars, suggesting an ``order-by-disorder'' mechanism in the Hilbert space. We give evidence for such scars and show their dynamical consequences on two-leg ladders with up to $56$ spins, which may be tested using available proposals of quantum simulators. Results on wider ladders point towards their presence in two dimensions as well.

arXiv comment8 pages (including Supplementary Material)

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