{"id":720760,"date":"2021-01-25T15:26:46","date_gmt":"2021-01-25T23:26:46","guid":{"rendered":"https:\/\/cm-edgetun.pages.dev\/en-us\/research\/?post_type=msr-research-item&#038;p=720760"},"modified":"2021-01-25T15:27:42","modified_gmt":"2021-01-25T23:27:42","slug":"exactly-solvable-model-for-a-4-1-d-beyond-cohomology-symmetry-protected-topological-phase","status":"publish","type":"msr-research-item","link":"https:\/\/cm-edgetun.pages.dev\/en-us\/research\/publication\/exactly-solvable-model-for-a-4-1-d-beyond-cohomology-symmetry-protected-topological-phase\/","title":{"rendered":"Exactly solvable model for a 4 +1 D beyond-cohomology symmetry-protected topological phase"},"content":{"rendered":"<p>We construct an exactly solvable commuting projector model for a $4+1$ dimensional ${\\mathbb Z}_2$ symmetry-protected topological phase (SPT) which is outside the cohomology classification of SPTs. The model is described by a decorated domain wall construction, with &#8220;three-fermion&#8221; Walker-Wang phases on the domain walls. We describe the anomalous nature of the phase in several ways. One interesting feature is that, in contrast to in-cohomology phases, the effective ${\\mathbb Z}_2$ symmetry on a $3+1$ dimensional boundary cannot be described by a quantum circuit and instead is a nontrivial quantum cellular automaton (QCA). A related property is that a codimension-two defect (for example, the termination of a ${\\mathbb Z}_2$ domain wall at a trivial boundary) will carry nontrivial chiral central charge $4$ mod $8$. We also construct a gapped symmetric topologically-ordered boundary state for our model, which constitutes an anomalous symmetry enriched topological phase outside of the classification of arXiv:1602.00187, and define a corresponding anomaly indicator.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We construct an exactly solvable commuting projector model for a $4+1$ dimensional ${\\mathbb Z}_2$ symmetry-protected topological phase (SPT) which is outside the cohomology classification of SPTs. The model is described by a decorated domain wall construction, with &#8220;three-fermion&#8221; Walker-Wang phases on the domain walls. We describe the anomalous nature of the phase in several ways. 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