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This research challenges the assumption that non-invertible symmetry protected topological phases lack symmetric entanglers by proving their existence in 1+1d systems via topological holography. The authors provide an explicit construction of such an entangler as a matrix product unitary for specific $\mathrm{Rep}(A_4)$-symmetry phases, offering a concrete counterexample to previous theoretical limitations. This advancement refines the understanding of quantum circuit structures connecting topological states, which is relevant for foundational work in quantum simulation and error correction.
Symmetric entanglers for non-invertible SPT phases
arXiv:2509.04581v3 Announce Type: replace-cross Abstract: It has been suggested that non-invertible symmetry protected topological phases (SPT), due to the lack of a stacking structure, do not have symmetric entanglers (globally symmetric finite-depth quantum circuits) connecting them. Using topological holography, we argue that a symmetric entangler should in fact exist for $1+1$d systems whenever the non-invertible symmetry has SPT phases connected by fixed-charge dualities (FCD). Moreover, we construct an explicit example of a symmetric entangler for the two SPT phases with $\mathrm{Rep}(A_4)$-symmetry, as a matrix product unitary (MPU).
Abstract:It has been suggested that non-invertible symmetry protected topological phases (SPT), due to the lack of a stacking structure, do not have symmetric entanglers (globally symmetric finite-depth quantum circuits) connecting them. Using topological holography, we argue that a symmetric entangler should in fact exist for $1+1$d systems whenever the non-invertible symmetry has SPT phases connected by fixed-charge dualities (FCD). Moreover, we construct an explicit example of a symmetric entangler for the two SPT phases with $\mathrm{Rep}(A_4)$-symmetry, as a matrix product unitary (MPU).
Strongly Correlated Electrons (cond-mat.str-el); High Energy Physics - Theory (hep-th); Quantum Physics (quant-ph)
arXiv:2509.04581 [cond-mat.str-el]
(or arXiv:2509.04581v3 [cond-mat.str-el] for this version)
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