Boundary-bulk relation in topological orders
Name
j.nuclphysb.2017.06.023_pdfa.pdf
Size
802.05 KB
Format
Adobe PDF
Checksum (MD5)
9482e15b257bcae2006ce2d88aad5e46
Author(s) • •
Kong, Liang
Zheng, Hao
Wen, Xiao-Gang
Date Issued
July 2017
Journal
Nuclear Physics B
Publisher
Elsevier
Citation
Kong, Liang, et al. “Boundary-Bulk Relation in Topological Orders.” Nuclear Physics B 922 (September 2017): 62–76 © 2017 The Author(s)
Version
Final published version
Abstract
In this paper, we study the relation between an anomaly-free n+1 D topological order, which are often called n+1 D topological order in physics literature, and its n D gapped boundary phases. We argue that the n+1 D bulk anomaly-free topological order for a given n D gapped boundary phase is unique. This uniqueness defines the notion of the “ bulk ” for a given gapped boundary phase. In this paper, we show that the n+1 D “ bulk ” phase is given by the “center” of the n D boundary phase. In other words, the geometric notion of the “ bulk ” corresponds precisely to the algebraic notion of the “center”. We achieve this by first introducing the notion of a morphism between two (potentially anomalous) topological orders of the same dimension, then proving that the notion of the “ bulk ” satisfies the same universal property as that of the “center” of an algebra in mathematics, i.e. “ bulk = center”. The entire argument does not require us to know the precise mathematical description of a (potentially anomalous) topological order. This result leads to concrete physical predictions.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution
Persistent DSpace Link
DOI of Published Version
https://doi.org/10.1016/j.nuclphysb.2017.06.023