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Detection of Symmetry Protected Topological Phases in 1D

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arxiv 1204.0704 v1 pith:OQTLEEYV submitted 2012-04-03 cond-mat.str-el

classification cond-mat.str-el
keywords ordersymmetryphasephasespointbeencannotcharacterized
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abstract

A topological phase is a phase of matter which cannot be characterized by a local order parameter. It has been shown that gapped phases in 1D systems can be completely characterized using tools related to projective representations of the symmetry groups. We show how to determine the matrices of these representations in a simple way in order to distinguish between different phases directly. From these matrices we also point out how to derive several different types of non-local order parameters for time reversal, inversion symmetry and $Z_2 \times Z_2$ symmetry, as well as some more general cases (some of which have been obtained before by other methods). Using these concepts, the ordinary string order for the Haldane phase can be related to a selection rule that changes at the critical point. We furthermore point out an example of a more complicated internal symmetry for which the ordinary string order cannot be applied.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Quantized topological invariant of symmetry-projected Gibbs states

    cond-mat.str-el 2026-08 conditional novelty 7.0 of 10

    Symmetry projection converts the thermally trivial 3D cluster model into a system with SPT, projected-paramagnetic, and disordered phases, distinguished by a quantized membrane invariant taking values -1, +1, and 0.

  2. Distinct finite-temperature phase diagrams of non-invertible Kennedy--Tasaki duals

    cond-mat.str-el 2026-07 accept novelty 7.0 of 10

    In three dimensions, a cluster-model interpolation and its non-invertible Kennedy–Tasaki dual have inequivalent finite-T phase diagrams over a finite window of the interpolation, proven exactly at s=0 and mapped by QMC.

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