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arXiv:1909.05868 · Physical review. B./Physical review. B

Multipolar topological field theories: Bridging higher order topological insulators and fractons

Yizhi You, F. J. Burnell, Taylor L. Hughes

Published Jun 16, 2021• 75 citations
arXivHTMLPDF

Abstract

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.

DOI
10.1103/physrevb.103.245128

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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 \( F[\phi] = r\phi^2 + u\phi^4 + \cdots \), broken symmetry group \( G \to H \); topological order: ground-state degeneracy \( \text{GSD} \sim e^{cL} \) (fractons) or \( \text{GSD} \sim L^g \) (toric code, \( g \) = genus); Chern–Simons action \( S_{CS} = \frac{k}{4\pi}\int \text{Tr}(A \wedge dA + \frac{2}{3}A^3) \); fracton gauge theory: \( S = \int (B_{ij}\partial_t A_{ij} - \text{...}) \) with symmetric tensor gauge fields \( A_{ij} \). | 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 \( C_4 \) rotational symmetry); the \( k \) 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

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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.
I discuss aspects of higher-order topological field theory of crystalline insulators with no other symmetries. I show how the topology and geometry of the crystalline lattice is organized in terms of so-called elasticity tetrads which are ground state degrees of freedom labelling translational lattice topological charges, higher-form conservation laws and responses on sub-dimensional manifolds of the bulk insulator. The quasitopological responses obtained in this way depend on the lattice and its embedding in space, as expected for weak topology. In a topological crystalline insulator, they classify higher-order responses and global symmetries in a transparent fashion in generic dimensions. This hierarchy coincides with the dimensional hierarchy of topological terms, the multipole expansion, and anomaly inflow, related to a mixed number of elasticity tetrads and electromagnetic gauge fields. In the continuum limit of the elasticity tetrads, the semi-classical expansion in momentum space can be used to derive the higher-order or subdimensional topological responses to local U(1) symmetries, such as electromagnetic gauge fields, with explicit formulas for the higher-order quasi-topological invariants in terms of the elasticity tetrads and Green’s functions. The topological responses in arbitrary dimensions are readily generalized to parameter space to allow for e.g. multipole pumping. The simple results further bridge the recently appreciated connections between topological field theory, higher-form symmetries and gauge fields and their relation to fractonic excitations and topological defects with restricted mobility in the elasticity of crystalline insulators.
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
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.
A time-reversal invariant topological insulator is defined by its topological magnetoelectric response that is robust against disorder. The response formula, defined on a Brillouin torus, defines a mathbbZ2mathbb{Z}_2mathbbZ2​ invariant and classifies the topological phase. However, in the presence of disorder or the magnetic field, the notion of Brillouin torus is destroyed and the response formula is no longer well-defined. This has been a challenging open problem, and it is essental in defining a topological insulator. This thesis proposes a topological response theory that is free from this fundamental deficiency. We derived the magnetoelectric response formula in position space for a generic three dimensional model under disorder and finite magnetic field. For time-reversal invariant systems, we connected the result to the 2nd Chern number in Noncommutative Geometry. We developed the noncommutative theory of Chern numbers and showed that the quantization of the magnetoelectric response is robust against disorder. Numerical studies on serveral disodered topological models in 1D and 3D are presented.
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: 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