Abstract
In this paper, we classify EF topological orders for 3+1D bosonic systems where some emergent pointlike excitations are fermions. (1) We argue that all 3+1D bosonic topological orders have gappable boundary. (2) All the pointlike excitations in EF topological orders are described by the representations of $G_f=Z_2^f\leftthreetimes_{e_2} G_b$ -- a $Z_2^f$ central extension of a finite group $G_b$ characterized by $e_2\in H^2(G_b,Z_2)$. (3) We find that the EF topological orders are classified by 2+1D anomalous topological orders $\mathcal{A}_b^3$ on their unique canonical boundary. Here $\mathcal{A}_b^3$ is a unitary fusion 2-category with simple objects labeled by $\hat G_b=Z_2^m\leftthreetimes G_b$. $\mathcal{A}_b^3$ also has one invertible fermionic 1-morphism for each object as well as quantum-dimension-$\sqrt 2$ 1-morphisms that connect two objects $g$ and $gm$, where $g\in \hat G_b$ and $m$ is the generator of $Z_2^m$. (4) When $\hat G_b$ is the trivial $Z_2^m$ extension, the EF topological orders are called EF1 topological orders, which is classified by simple data $(G_b,e_2,n_3,\nu_4)$. (5) When $\hat G_b$ is a non-trivial $Z_2^m$ extension, the EF topological orders are called EF2 topological orders, where some intersections of three stringlike excitations must carry Majorana zero modes. (6) Every EF2 topological order with $G_f=Z_2^f\leftthreetimes G_b$ can be associated with a EF1 topological order with $G_f=Z_2^f\leftthreetimes \hat G_b$. (7) We find that all EF topological orders correspond to gauged 3+1D fermionic symmetry protected topological (SPT) orders with a finite unitary symmetry group. (8) We further propose that the general classification of 3+1D topological orders with finite unitary symmetries for bosonic and fermionic systems can be obtained by gauging or partially gauging the finite symmetry group of 3+1D SPT phases of bosonic and fermionic systems.
Highlights
The study of topological phases of matter has become a very active field in condensed-matter physics
The 2 þ 1D topological order is mathematically described by fusion categories, whose objects correspond to pointlike excitations, and morphisms correspond to physical processes, such as braiding
(7) We find that all EF topological orders correspond to gauged 3 þ 1D fermionic symmetry-protected topological (SPT) orders with a finite unitary symmetry group
Summary
The study of topological phases of matter has become a very active field in condensed-matter physics. We classify 3 þ 1D topological orders whose emergent pointlike excitations are bosons and fermions, which are called EF topological orders. [37] and in this paper classify all 3 þ 1D topological orders in bosonic systems, since there are only two kinds of statistics for pointlike excitations in 3 þ 1D: Bose statistics and Fermi statistics. Since the remote detection is done by braiding, the self-consistency of fusion and braiding plus the remote detectability can totally fix the structure of pointlike and stringlike excitations Those structures, in turn, classify the 3 þ 1D EF topological orders
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