A degeneracy bound for homogeneous topological order
arXiv:2009.13551 · doi:10.21468/SciPostPhys.10.1.011
Abstract
We introduce a notion of homogeneous topological order, which is obeyed by most, if not all, known examples of topological order including fracton phases on quantum spins (qudits). The notion is a condition on the ground state subspace, rather than on the Hamiltonian, and demands that given a collection of ball-like regions, any linear transformation on the ground space be realized by an operator that avoids the ball-like regions. We derive a bound on the ground state degeneracy for systems with homogeneous topological order on an arbitrary closed Riemannian manifold of dimension , which reads \[ \log \mathcal D \le c μ(L/a)^{d-2}.\] Here, is the diameter of the system, is the lattice spacing, and is a constant that only depends on the isometry class of the manifold, and is a constant that only depends on the density of degrees of freedom. If , the constant is the (demi)genus of the space manifold. This bound is saturated up to constants by known examples.
arXiv comment12 pages, 2 figures (v2) clarified the main theorem for d=2, added some detail for Pauli stabilizer models, (v3) minor corrections
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- Bifurcating subsystem symmetric entanglement renormalization in two dimensions
- Fractons on Graphs and Complexity
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- Layer Codes
- Lift-Connected Surface Codes
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- Fractons on the edge
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- Entanglement renormalization of fractonic anisotropic Laplacian models