Exactly solvable topological phase transition in a quantum dimer model
- URL: http://arxiv.org/abs/2601.15377v1
- Date: Wed, 21 Jan 2026 19:00:01 GMT
- Title: Exactly solvable topological phase transition in a quantum dimer model
- Authors: Laura Shou, Jeet Shah, Matthew Lerner-Brecher, Amol Aggarwal, Alexei Borodin, Victor Galitski,
- Abstract summary: We study a quantum dimer model on the triangular lattice, with doubly-periodic edge weights.<n>We explain the constant vison correlator in terms of loops statistics of the double-dimer model.
- Score: 0.013434289790264115
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: We introduce a family of generalized Rokhsar-Kivelson (RK) Hamiltonians, which are reverse-engineered to have an arbitrary edge-weighted superposition of dimer coverings as their exact ground state at the RK point. We then focus on a quantum dimer model on the triangular lattice, with doubly-periodic edge weights. For simplicity we consider a $2\times1$ periodic model in which all weights are set to one except for a tunable horizontal edge weight labeled $α$. We analytically show that the model exhibits a continuous quantum phase transition at $α=3$, changing from a topological $\mathbb{Z}_2$ quantum spin liquid ($α<3$) to a columnar ordered state ($α>3$). The dimer-dimer correlator decays exponentially on both sides of the transition with the correlation length $ξ\propto1/|α-3|$ and as a power-law at criticality. The vison correlator exhibits an exponential decay in the spin liquid phase, but becomes a constant in the ordered phase. We explain the constant vison correlator in terms of loops statistics of the double-dimer model. Using finite-size scaling of the vison correlator, we extract critical exponents consistent with the 2D Ising universality class.
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