Generating domain walls between topologically ordered phases using quantum double models

TL;DR

This paper introduces exactly solvable quantum double models that dynamically generate domain walls between topologically ordered phases, revealing new properties like anyon fusion, permutation, and potential ground state degeneracies.

Contribution

It presents a novel class of models where domain walls are part of the spectrum, enabling study of their properties without artificial boundary creation.

Findings

Domain walls can fuse with anyons to create or annihilate them.

Domain walls can permute anyons, acting as synthetic scatterers.

Models exhibit ground state degeneracy from symmetry breaking and topological order.

Abstract

Transitions between different topologically ordered phases have been studied by artificially creating boundaries between these gapped phases and thus studying their effects relating to condensation and tunneling of particles from one phase to the other. In this work we introduce exactly solvable models which are similar to the quantum double models (QDM) of Kitaev where such domain walls are dynamically generated making them a part of the spectrum. These systems have a local symmetry and may or may not have a global symmetry leading to the possibility of a ground state degeneracy arising from both, global symmetry breaking and a topological degeneracy. The domain wall states now separate the different topologically ordered phases belonging to the different sectors controlled by the global symmetry, when present. They have interesting properties including fusion with the deconfined anyons of the topologically ordered phase, to either create new domain walls, or their annihilation. They can also act like a scatterer permuting anyons of the topologically ordered phases on either side of the domain wall. Thus these domain wall states can be thought of as a synthetic scatterer which can be created in any part of the lattice. We show these effects for the simplest case of the $\mathbb{Z}_2$ toric code phase decorated with a global $\mathbb{Z}_2$ symmetry and then make remarks about the case when we have the QDM based on two arbitrary groups $G_1$ and $G_2$ in which case we may no longer have a global symmetry.