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Quantized electric multipole insulators

TLDR
This work introduces a paradigm in which “nested” Wilson loops give rise to topological invariants that have been overlooked and opens a venue for the expansion of the classification of topological phases of matter.
Abstract
The Berry phase provides a modern formulation of electric polarization in crystals. We extend this concept to higher electric multipole moments and determine the necessary conditions and minimal models for which the quadrupole and octupole moments are topologically quantized electromagnetic observables. Such systems exhibit gapped boundaries that are themselves lower-dimensional topological phases. Furthermore, they host topologically protected corner states carrying fractional charge, exhibiting fractionalization at the boundary of the boundary. To characterize these insulating phases of matter, we introduce a paradigm in which “nested” Wilson loops give rise to topological invariants that have been overlooked. We propose three realistic experimental implementations of this topological behavior that can be immediately tested. Our work opens a venue for the expansion of the classification of topological phases of matter.

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Observation of higher-order non-Hermitian skin effect

TL;DR: In this paper, the spin-polarized, higher-order non-Hermitian skin effect in two-dimensional (2D) acoustic metamaterials was demonstrated using a lattice of coupled whisper gallery acoustic resonators.
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Quadrupole topological photonic crystals

TL;DR: In this article, the authors identify the analog of quadrupole order in Maxwell's equations for a gyromagnetic photonic crystal (PhC) through a double-band-inversion process.
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Higher-order topological insulators in amorphous solids

TL;DR: In this article, it was shown that crystalline topological phases can be materialized in non-crystalline systems and that when weak structural disorder is confined within the interior of the system, it can support amorphous higher-order topological insulators.
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Fractional disclination charge in two-dimensional C n -symmetric topological crystalline insulators

TL;DR: In this article, the fractional charge on disclinations in Ω(n)-symmetric 2D topological crystalline insulators (TCIs) was investigated, with or without time-reversal symmetry, and including spinless and spin-$\frac{1}{2}$ cases.
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Non-Abelian band topology in noninteracting metals.

TL;DR: In this article, the authors introduced non-Abelian topological charges that characterize line nodes inside the momentum space of crystalline metals with space-time inversion (𝒫𝒯) symmetry and with weak spin-orbit coupling.
References
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Journal ArticleDOI

New Method for High-Accuracy Determination of the Fine-Structure Constant Based on Quantized Hall Resistance

TL;DR: In this article, the Hall voltage of a two-dimensional electron gas, realized with a silicon metal-oxide-semiconductor field effect transistor, was measured and it was shown that the Hall resistance at particular, experimentally well-defined surface carrier concentrations has fixed values which depend only on the fine-structure constant and speed of light, and is insensitive to the geometry of the device.
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Quantized Hall conductance in a two-dimensional periodic potential

TL;DR: In this article, the Hall conductance of a two-dimensional electron gas has been studied in a uniform magnetic field and a periodic substrate potential, where the Kubo formula is written in a form that makes apparent the quantization when the Fermi energy lies in a gap.
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Model for a Quantum Hall Effect without Landau Levels: Condensed-Matter Realization of the 'Parity Anomaly'

TL;DR: A two-dimensional condensed-matter lattice model is presented which exhibits a nonzero quantization of the Hall conductance in the absence of an external magnetic field, and exhibits the so-called "parity anomaly" of (2+1)-dimensional field theories.
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Maximally localized generalized Wannier functions for composite energy bands

TL;DR: In this paper, a method for determining the optimally localized set of generalized Wannier functions associated with a set of Bloch bands in a crystalline solid is presented, which is suitable for use in connection with conventional electronic-structure codes.
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Theory of polarization of crystalline solids

TL;DR: It is shown that physically $\ensuremath{\Delta}P can be interpreted as a displacement of the center of charge of the Wannier functions.
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