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Monte Carlo analysis of critical phenomenon of the Ising model on memory stabilizer structures

Source: Phys. Rev. A 80, 042313 (2009); doi:10.1103/PhysRevA.80.042313

Published 19 October 2009

KEYWORDS and PACS
Keywords
PACS
  • 03.67.Lx
    Quantum computation architectures and implementations
  • 03.67.Pp
    Quantum error correction and other methods for protection against decoherence
  • 64.60.an
    Finite-size system studies of phase transitions
  • 64.60.De
    Statistical mechanics of model systems (phase transitions)
  • YEAR: 2009
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
C. Ricardo Viteri, Yu Tomita, and Kenneth R. Brown
School of Chemistry and Biochemistry and Computational Science and Engineering Division, Georgia Institute of Technology, Atlanta, Georgia 30332, USA
We calculate the critical temperature of the Ising model on a set of graphs representing a concatenated three-bit error-correction code. The graphs are derived from the stabilizer formalism used in quantum error correction. The stabilizer for a subspace is defined as the group of Pauli operators whose eigenvalues are +1 on the subspace. The group can be generated by a subset of operators in the stabilizer, and the choice of generators determines the structure of the graph. The Wolff algorithm, together with the histogram method and finite-size scaling, is used to calculate both the critical temperature and the critical exponents of each structure. The simulations show that the choice of stabilizer generators, both the number and the geometry, has a large effect on the critical temperature. ©2009 The American Physical Society
History: Received 1 July 2009; published 19 October 2009
Permalink: http://link.aps.org/abstract/PRA/v80/e042313
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