Symmetry protected topological (SPT) states have boundary 't Hooft anomalies
that obstruct an effective boundary theory realized in its own dimension with
UV completion and an on-site G-symmetry. In this work, yet we show that a
certain anomalous non-on-site G symmetry along the boundary becomes on-site
when viewed as an extended H symmetry, via a suitable group extension 1→K→H→G→1. Namely, a non-perturbative global (gauge/gravitational)
anomaly in G becomes anomaly-free in H. This guides us to construct exactly
soluble lattice path integral and Hamiltonian of symmetric gapped boundaries,
always existent for any SPT state in any spacetime dimension d≥2 of any
finite symmetry group, including on-site unitary and anti-unitary time-reversal
symmetries. The resulting symmetric gapped boundary can be described either by
an H-symmetry extended boundary of bulk d≥2, or more naturally by a
topological emergent K-gauge theory with a global symmetry G on a 3+1D bulk
or above. The excitations on such a symmetric topologically ordered boundary
can carry fractional quantum numbers of the symmetry G, described by
representations of H. (Apply our approach to a 1+1D boundary of 2+1D bulk, we
find that a deconfined gauge boundary indeed has spontaneous symmetry breaking
with long-range order. The deconfined symmetry-breaking phase crosses over
smoothly to a confined phase without a phase transition.) In contrast to known
gapped interfaces obtained via symmetry breaking (either global symmetry
breaking or Anderson-Higgs mechanism for gauge theory), our approach is based
on symmetry extension. More generally, applying our approach to SPT,
topologically ordered gauge theories and symmetry enriched topologically
ordered (SET) states, leads to generic boundaries/interfaces constructed with a
mixture of symmetry breaking, symmetry extension, and dynamical gauging.Comment: 144 pages, 29 figures, 22 tables. v3: Refinement/Refs added.
Un/Trimmed version on arXiv/PR