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Title: Topological quantum order: Stability under local perturbations

Journal Article · · Journal of Mathematical Physics
DOI:https://doi.org/10.1063/1.3490195· OSTI ID:21476500
 [1];  [2];  [3]
  1. IBM Watson Research Center, Yorktown Heights, New York 10594 (United States)
  2. Microsoft Research Station Q, CNSI Building, University of California, Santa Barbara, California 93106 (United States)
  3. T-4 and CNLS, LANL, Los Alamos, New Mexico 87544 (United States)

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 H{sub 0}, we prove that there exists a constant threshold {epsilon}>0 such that for any perturbation V representable as a sum of short-range bounded-norm interactions, the perturbed Hamiltonian H=H{sub 0}+{epsilon}V has well-defined spectral bands originating from low-lying eigenvalues of H{sub 0}. 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 H{sub 0} 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.

OSTI ID:
21476500
Journal Information:
Journal of Mathematical Physics, Vol. 51, Issue 9; Other Information: DOI: 10.1063/1.3490195; (c) 2010 American Institute of Physics; ISSN 0022-2488
Country of Publication:
United States
Language:
English