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arXiv:2010.08917 · Physical review. B./Physical review. B

Fractonic order in infinite-component Chern-Simons gauge theories

Xiuqi Ma, Wilbur E. Shirley, Meng Cheng, Michael Levin, John McGreevy, Xie Chen

Published May 18, 2022• 25 citations
arXivHTMLPDF

Abstract

The Chern-Simons theory is a powerful tool in the study of 2+1D topological phases, especially quantum Hall systems. Here, the authors extend the framework by allowing an infinite number of gauge fields and use it to study the 3+1D fracton order. Fracton order has been studied mostly using lattice models and higher-rank gauge theories. The introduction of the Chern-Simons formulation allows the user to take advantage of theoretical tools developed over the past decades for quantum Hall systems. In particular, the authors are able to study foliated fracton order more systematically and identify a new type of fracton order, not possible in previous formulations.

DOI
10.1103/physrevb.105.195124

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The Chern-Simons theory is a powerful tool in the study of 2+1D topological phases, especially quantum Hall systems. Here, the authors extend the framework by allowing an infinite number of gauge fields and use it to study the 3+1D fracton order. Fracton order has been studied mostly using lattice models and higher-rank gauge theories. The introduction of the Chern-Simons formulation allows the user to take advantage of theoretical tools developed over the past decades for quantum Hall systems. In particular, the authors are able to study foliated fracton order more systematically and identify a new type of fracton order, not possible in previous formulations.
Fracton order is an intriguing new type of order which shares many common features with topological order, such as topology-dependent ground-state degeneracies, and excitations with mutual statistics.However, it also has several distinctive geometrical aspects, such as excitations with restricted mobility, which naturally lead to effective descriptions in terms of higher-rank gauge fields.In this paper, we investigate possible effective field theories for three-dimensional fracton order, by presenting a general philosophy whereby topological-like actions for such higher-rank gauge fields can be constructed.Our approach draws inspiration from Chern-Simons and BF theories in 2+1 dimensions, and imposes constraints binding higher-rank gauge charge to higher-rank gauge flux.We show that the resulting fractonic Chern-Simons and BF theories reproduce many of the interesting features of their familiar two-dimensional cousins.We analyze one example of the resulting fractonic Chern-Simons theory in detail, and show that upon quantization it realizes a gapped fracton order with quasiparticle excitations that are mobile only along a subset of one-dimensional lines, and display a form of fractional self-statistics.The ground-state degeneracy of this theory is both topology and geometry dependent, scaling exponentially with the linear system size when the model is placed on a three-dimensional torus.By studying the resulting quantum theory on the lattice, we show that it describes a Z s generalization of the Chamon code.
FINDING: Fractonic Chern-Simons theory extends topological gauge theory to higher-rank symmetric tensor gauge fields, enabling fracton phases with restricted mobility and subdimensional topological order. | MATH: Higher-rank gauge fields: Aij A_{ij} Aij​ (symmetric tensor) with gauge transformation δAij=∂i∂jα \delta A_{ij} = \partial_i \partial_j \alpha δAij​=∂i​∂j​α; fractonic Chern-Simons action: S=k4π∫ϵμνρAμ∂νAρ S = \frac{k}{4\pi} \int \epsilon^{\mu\nu\rho} A_{\mu} \partial_\nu A_{\rho} S=4πk​∫ϵμνρAμ​∂ν​Aρ​ generalized to higher-rank; fracton charge conservation: ∂i∂jJij=0 \partial_i \partial_j J_{ij} = 0 ∂i​∂j​Jij​=0; dipole moment conservation: ∫xiρ \int x^i \rho ∫xiρ constant. | CONNECTION: Crystallographic group symmetries (e.g., cubic, hexagonal) constrain allowed higher-rank tensor gauge fields; lattice structures (e.g., square, triangular) yield subdimensional particle mobility; no direct golden ratio or base-60 link found. | DEPTH: 8 — Fractonic Chern-Simons theory unifies higher-rank gauge theory with topological order, revealing new quantum phase Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Topological order and fracton phases transcend the Landau paradigm, requiring non-local, categorical and higher-form gauge-theoretic descriptions rather than symmetry-breaking order parameters. | MATH: Landau theory: free energy F[ϕ]=rϕ2+uϕ4+⋯ F[\phi] = r\phi^2 + u\phi^4 + \cdots F[ϕ]=rϕ2+uϕ4+⋯, broken symmetry group G→H G \to H G→H; topological order: ground-state degeneracy GSD∼ecL \text{GSD} \sim e^{cL} GSD∼ecL (fractons) or GSD∼Lg \text{GSD} \sim L^g GSD∼Lg (toric code, g g g = genus); Chern–Simons action SCS=k4π∫Tr(A∧dA+23A3) S_{CS} = \frac{k}{4\pi}\int \text{Tr}(A \wedge dA + \frac{2}{3}A^3) SCS​=4πk​∫Tr(A∧dA+32​A3); fracton gauge theory: S=∫(Bij∂tAij−...) S = \int (B_{ij}\partial_t A_{ij} - \text{...}) S=∫(Bij​∂t​Aij​−...) with symmetric tensor gauge fields Aij A_{ij} Aij​. | CONNECTION: Fracton phases exhibit sub-dimensional particle motion — point excitations confined to lines or planes — mirroring the geometry of root systems and lattice symmetries (e.g., cubic lattices with C4 C_4 C4​ rotational symmetry); the k k k level in Chern–Simons theory is quantized (integer), linking to mo Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
The concepts of multipolar insulators and multipole symmetries have hinted at tantalizing connections between the disparate fields of higher-order topological insulators and fracton phases. Here, the authors show that these connections are not superficial, but instead arise from a unified field theory description of the topological response of these systems to external fields, similar to the quantized Hall conductance of Chern insulators, and the quantized axion magnetoelectric polarizability in 3D topological insulators. These response theories are built from the recently introduced higher-rank tensor gauge potentials, and can be interpreted, in some scenarios, as the topological response to ordinary electric and magnetic field gradients.
We introduce a generalization of conventional lattice gauge theory to describe fracton topological phases, which are characterized by immobile, pointlike topological excitations, and subextensive topological degeneracy. We demonstrate a duality between fracton topological order and interacting spin systems with symmetries along extensive, lower-dimensional subsystems, which may be used to systematically search for and characterize fracton topological phases. Commutative algebra and elementary algebraic geometry provide an effective mathematical tool set for our results. Our work paves the way for identifying possible material realizations of fracton topological phases.
We broaden the scope of quantum field theory by introducing a general class of discrete gauge theories that realize either topological order or fracton behavior across dimensions. We start from translation-invariant systems endowed with unconventional charge-conservation laws, which we term \textit{exponential polynomial symmetries}. Gauging these symmetries yields ZN\mathbb{Z}_NZN​ gauge theories in 2D that exhibit topological order whose quasiparticles have constrained mobility and whose ground-state degeneracy shows ultraviolet (UV) dependence. These features are reminiscent of spatial symmetry-enriched topological order, wherein quasiparticle excitations transform nontrivially under lattice translations. We further propose a Chern-Simons variant that produces non-CSS stabilizer codes and outline a framework for exponentially symmetric subsystem SPT phases. Finally, we extend this gauging procedure to 3D, obtaining new variants of fracton topological order.