Invariants for Gapped Ground State Phases
summary
States with a uniform spectral gap map to each other by a quasi-local quasi-adiabatic continuation (spectral flow) that commutes with on-site symmetry, so the symmetry representation on a half-infinite chain is constant along any gapped path. For 1D frustration-free matrix product ground states the transfer map has a simple eigenvalue 1 and a transfer operator gap giving exponential convergence, which lets one construct a cutoff-weighted generator and a well-defined boundary representation (AKLT: bulk spin-1 → two-dimensional spin-1/2 edge), hence a computable bulk invariant.
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chapters (22)
- 0:00Introduction
- 0:12Symmetry protected phases
- 5:50Defining ground state phases
- 9:11Limits of ground states
- 11:05Role of invariants
- 14:00Detecting phase transitions
- 16:28Understanding level crossing
- 17:38Local symmetry properties
- 20:53AKLT model example
- 24:16Adiabatic evolution
- 26:43Equivalence of ground states
- 30:06AKLT boundary states
- 33:41Symmetry in AKLT
- 35:30Detecting invariants
- 37:25MPS ground states
- 38:40MPS formalism review
- 44:10Properties of the map
- 47:20Bulk calculation
- 50:30Defining symmetry action
- 55:13Calculation theorem
- 1:00:14Final results
- 1:03:44Extensions and closing
