Artigo Acesso aberto Revisado por pares

Topological quantum order: Stability under local perturbations

2010; American Institute of Physics; Volume: 51; Issue: 9 Linguagem: Inglês

10.1063/1.3490195

ISSN

1527-2427

Autores

Sergey Bravyi, Matthew B. Hastings, Spyridon Michalakis,

Tópico(s)

Quantum and electron transport phenomena

Resumo

We study zero-temperature stability of topological phases of matter under weak time-independent perturbations. Our results apply to quantum spin Hamiltonians that can be written as a sum of geometrically local commuting projectors on a D-dimensional lattice with certain topological order conditions. Given such a Hamiltonian H0, we prove that there exists a constant threshold ϵ>0 such that for any perturbation V representable as a sum of short-range bounded-norm interactions, the perturbed Hamiltonian H=H0+ϵV has well-defined spectral bands originating from low-lying eigenvalues of H0. These bands are separated from the rest of the spectra and from each other by a constant gap. The band originating from the smallest eigenvalue of H0 has exponentially small width (as a function of the lattice size). Our proof exploits a discrete version of Hamiltonian flow equations, the theory of relatively bounded operators, and the Lieb–Robinson bound.

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