Exactly solvable model for a deconfined quantum critical point in 1D
arXiv:2206.01222 · doi:10.1103/PhysRevLett.130.026801
Abstract
We construct an exactly solvable lattice model for a deconfined quantum critical point (DQCP) in (1+1) dimensions. This DQCP occurs in an unusual setting, namely at the edge of a (2+1) dimensional bosonic symmetry protected topological phase (SPT) with symmetry. The DQCP describes a transition between two gapped edges that break different subgroups of the full symmetry. Our construction is based on an exact mapping between the SPT edge theory and a spin chain. This mapping reveals that DQCPs in this system are directly related to ordinary symmetry breaking critical points.
arXiv comment4.25 pages with 3 figures + 3 page supplemental material with 1 figure. References, discussion, and intro updated
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