2019/12/31 by Zheyan Wan, Juven Wang, Yunqin Zheng
Physics and Astronomy · Mathematics · #hep-th #cond-mat.str-el #hep-ph #math.AT
paper · pdf · doi:10.4310/amsa.2020.v5.n2.a2
published as Annals of Mathematical Sciences and Applications, Vol. 5, No. 2, 171-257 (2020) · Sequel to: arXiv:1711.11587, arXiv:1812.11967, arXiv:1904.00994 arXiv:1910.14668, arXiv:1912.13514. Accepted by Annals of Mathematical Sciences and Applications, Vol. 5, No. 2 (2020)
arxiv created 2020/09/03 · arxiv updated 2020/10/14
We systematically study Lorentz symmetry extensions in quantum field theories (QFTs) and their 't Hooft anomalies via cobordism. The total symmetry G' can be expressed in terms of the extension of Lorentz symmetry GL by an internal global symmetry G as 1 → G → G' → GL → 1. By enumerating all possible GL and symmetry extensions, other than the familiar SO/Spin/O/Pin± groups, we introduce a new EPin group (in contrast to DPin), and provide natural physical interpretations to exotic groups E(d), EPin(d), (SU(2)×E(d))/ℤ2, (SU(2)×EPin(d))/ℤ2±, etc. By Adams spectral sequence, we systematically classify all possible dd Symmetry Protected Topological states (SPTs as invertible TQFTs) and (d-1)d 't Hooft anomalies of QFTs by co/bordism groups and invariants in d≤ 5. We further gauge the internal G, and study Lorentz symmetry-enriched Yang-Mills theory with discrete theta terms given by gauged SPTs. We not only enlist familiar bosonic Yang-Mills but also discover new fermionic Yang-Mills theories (when GL contains a graded fermion parity ℤ2F), applicable to bosonic (e.g., Quantum Spin Liquids) or fermionic (e.g., electrons) condensed matter systems. For a pure gauge theory, there is a one form symmetry I[1] associated with the center of the gauge group G. We further study the anomalies of the emergent symmetry I[1]× GL by higher cobordism invariants as well as QFT analysis. We focus on the simply connected G=SU(2) and briefly comment on non-simply connected G=SO(3), U(1), other simple Lie groups, and Standard Model gauge groups (SU(3)×SU(2)×U(1))/ℤq. We comment on SPTs protected by Lorentz symmetry, and the symmetry-extended trivialization for their boundary states.