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Volume and topological invariants of quantum many-body systems

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PhysRevResearch.2.033030.pdf

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sword-2021-07-12T12:26:29.original.xml (130 B)
Original SWORD entry document
Author(s)
Wen, Xiao-Gang
•
Wang, Zhenghan
Date Issued
2020
Journal
Physical Review Research
Publisher
American Physical Society (APS)
Version
Final published version
Abstract
A gapped many-body system is described by path integral on a space-time lattice $C^{d+1}$, which gives rise to a partition function $Z(C^{d+1})$ if $\partial C^{d+1} =\emptyset$, and gives rise to a vector $|\Psi\rangle$ on the boundary of space-time if $\partial C^{d+1} \neq\emptyset$. We show that $V = \text{log} \sqrt{\langle\Psi|\Psi\rangle}$ satisfies the inclusion-exclusion property $\frac{V(A\cup B)+V(A\cap B)}{V(A)+V(B)}=1$ and behaves like a volume of the space-time lattice $C^{d+1}$ in large lattice limit (i.e. thermodynamics limit). This leads to a proposal that the vector $|\Psi\rangle$ is the quantum-volume of the space-time lattice $C^{d+1}$. The inclusion-exclusion property does not apply to quantum-volume since it is a vector. But quantum-volume satisfies a quantum additive property. The violation of the inclusion-exclusion property by $V = \text{log} \sqrt{\langle\Psi|\Psi\rangle}$ in the subleading term of thermodynamics limit gives rise to topological invariants that characterize the topological order in the system. This is a systematic way to construct and compute topological invariants from a generic path integral. For example, we show how to use non-universal partition functions $Z(C^{2+1})$ on several related space-time lattices $C^{2+1}$ to extract $(M_f)_{11}$ and $\text{Tr}(M_f)$, where $M_f$ is a representation of the modular group $SL(2,\mathbb{Z})$ -- a topological invariant that almost fully characterizes the 2+1D topological orders.
MIT Department
Massachusetts Institute of Technology. Department of Physics
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Creative Commons Attribution 4.0 International license
https://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
https://hdl.handle.net/1721.1/135487
DOI of Published Version
https://doi.org/10.1103/PHYSREVRESEARCH.2.033030
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