Abstract

We explore 4d Yang-Mills gauge theories (YM) living as boundary conditions of 5d gapped short/long-range entangled (SRE/LRE) topological states. Specifically, we explore 4d time-reversal symmetric pure YM of an SU(2) gauge group with a second-Chern-class topological term at $\theta=\pi$ (SU(2)$_{\theta=\pi}$ YM), by turning on background fields for both the time-reversal (i.e., on unorientable manifolds) and 1-form center global symmetry. We find four classes of time-reversal and Lorentz symmetry-enriched SU(2)$_{\theta=\pi}$ YM, labeled by $(K_1, K_2)$: $K_1=0,1$ specifies Kramers singlet/doublet Wilson line and new mixed higher 't Hooft anomalies; $K_2=0,1$ specifies boson/fermionic Wilson line and a new Wess-Zumino-Witten-like counterterm. Higher anomalies indicate that to realize all higher $n$-global symmetries locally on $n$-simplices, the 4d theory becomes a boundary of a 5d higher-symmetry-protected topological state (SPTs, as an invertible topological quantum field theory (TQFT) or a cobordism invariant in math, or as a 5d higher-symmetric interacting topological superconductor in condensed matter). By dynamically gauging the 1-form symmetry, we transform a 5d bulk SRE SPTs into an LRE symmetry-enriched topologically ordered state (SETs); thus we obtain the 4d SO(3)$_{\theta=\pi}$ YM-5d LRE-higher-SETs coupled system with higher-form gauge fields. We further derive new exotic anyonic statistics of extended objects such as 2-worldsheet of strings and 3-worldvolume of branes, physically characterizing the 5d SETs. We discover triple and quadruple link invariants associated with the 5d higher-gauge TQFTs, hinting at a relation between non-supersymmetric 4d pure YM and topological links in 5d. We provide 4d-5d lattice simplicial complex regularizations and bridge to 4d quantum spin liquids. We constrain gauge dynamics by higher anomalies and a higher symmetry-extension method.

Highlights

  • AND SUMMARYThe world where we reside, to our best present understanding, can be described by quantum theory and the underlying long-range entanglement

  • We explore various 4d Yang-Mills gauge theories (YM) living as boundary conditions of 5d gapped short-/long-range entangled (SRE/LRE) topological states

  • We discover triple and quadruple link invariants potentially associated with the underlying 5d higher-gauge topological quantum field theories, hinting at a new intrinsic relation between nonsupersymmetric 4d pure YM and topological links in 5d

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Summary

INTRODUCTION

The world where we reside, to our best present understanding, can be described by quantum theory and the underlying long-range entanglement. We comment on the physical and mathematical meanings of fractional statistics and non-Abelian statistics associated with the spacetime braiding processes involving 0D anyonic particles, 1D anyonic strings, 2D anyonic branes, and other extended objects. (ii) In our generalized definition, anyonic means that either self-exchange statistics (of identical objects) or the mutual statistics (of multiple distinguishable objects, may involving more than two objects) can go beyond bosonic or fermionic statistics.—In 3d (2 þ 1D) spacetime M 3 , braiding statistics of particles can be fractional (such as the exchange statistics of two identical particles, or mutual statistics of two different particles) which are called anyonic particles (see an excellent historical overview [17]) As an example, this can be understood from a 3d Chern-Simons action with one-form gauge field a integrated over M 3. (4) Section VI.—We provide the exemplary spacetime braiding processes of anyonic string/brane in 5d, and the link configurations of extended operators, which

The Outline
Summaries and Tables
Ordinary and higher global symmetries of Yang-Mills theory
Identifying Sanom with 5d cobordism group data
Anomaly matching of 4d–5d inflow
Topological term on torsion-free orientable manifolds
Consequences and interpretations of four siblings of “anomalies”
On a closed manifold
On a manifold with a boundary
Enumeration of gauge theories from dynamically gauging 4d SPTs
Partition function of 5d higher-gauge TQFTs ð3:17Þ
Partition function and topological degeneracy
Bþð1þK Þw ðTMÞ2 Sq1 Bþw ðTMÞSq1 B
Computation
Version I: w1 ðTMÞ3 B and a quartic link invariant
Gauge invariance
Lattice realization of 4d higher SPTs and higher-gauge TQFT
Lattice realization of 5d higher SPTs and higher-gauge SETs
Higher-symmetry-extended
Full Text
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