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Symmetrization of topologically ordered wavefunctions is a powerful method for constructing new topological models.
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K. Duivenvoorden, M. Iqbal, J. Haegeman, F. Verstraete, and N. Schuch, in preparation
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Note that the converse is not true: There can be tensors of the form Eq. ( 1
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Note that the largest eigenvalue of the transfer operator for the normalization ⟨ ψ 4 a | ψ 4 a ⟩ \delimiter 69632778\psi_{4a}\delimiter 2532108\psi_{4a}\delimiter 86414091 of the non-abelian anyon 4 a 4a is degenerate, which allows it to have non-zero overlap with more than one sector (while without such a degeneracy, i.e., for abelian anyons, the normalized overlap must always be zero or one)
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