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Unconventional topological edge states in one-dimensional gapless systems stemming from nonisolated hypersurface singularities

Mesoscale and Nanoscale Physics · Submitted 5 Mar 2025

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Unexpectedly, such gapless systems still afford topologically protected edge states at system boundaries, challenging the conventional understanding based on band gaps.

how it is stated · asserted 1.00 read the record →

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arXiv ID2503.03314 (version 1)
Pith IDDE7T2KSY, Pith's permanent record of this paper and its review
CitationC. T. Chan, Dongyang Wang, Hongwei Jia, Jing Hu, Mudi Wang, Ruo-Yang Zhang, Shaojie Ma, Xiaoping Ouyang, Yifei Zhu, Yixin Xiao. "Unconventional topological edge states in one-dimensional gapless systems stemming from nonisolated hypersurface singularities." arXiv:2503.03314 (2025). https://pith.science/paper/DE7T2KSY
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 6,422 input tokens.

What the abstract itself states, as probabilities: claims first 0.85 · states limitation 0.12 · human participants 0.02 · controlled comparison 0.09 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.92 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

Topologically protected edge states have been extensively studied in systems characterized by the topological invariants in band gaps (also called line gaps). In this study, we unveil a whole new form of edge states that transcends the established paradigms of band-gap topology. In contrast to the traditional stable edge states in topological insulators with specific band gaps, the one-dimensional systems we investigate are inherently gapless with the Brillouin zones being mapped to the loops encircling hypersurface singularities in a higher-dimensional space with parity-time symmetry. These hypersurface singularities are nonisolated degeneracies embedded entirely on exceptional surfaces, rendering the energy gaps in our systems inevitably closed at the intersections of the Brillouin zone loop and the exceptional surfaces. Unexpectedly, such gapless systems still afford topologically protected edge states at system boundaries, challenging the conventional understanding based on band gaps. To elucidate the existence of these edge states in the absence of a band-gap-based invariant, we propose a theoretical framework based on eigen-frame rotation and deformation that incorporates non-Bloch band theory. Finally, we experimentally demonstrate this new form of topological edge states with nonreciprocal circuits for the first time. Our work constitutes a major advance that extends topological edge states from gapped phases to gapless phases, offering new insights into topological phenomena.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Topologically protected edge states have been extensively studied in systems characterized by the topological invariants in band gaps (also called line gaps). background 1.00 0.04 0.02 asserted 1.00
s1 In this study, we unveil a whole new form of edge states that transcends the established paradigms of band-gap topology. contribution 0.97 0.91 0.23 asserted 1.00
s2 In contrast to the traditional stable edge states in topological insulators with specific band gaps, the one-dimensional systems we investigate are inherently gapless with the Brillouin zones being mapped to the loops encircling hypersurface singularities in a higher-dimensional space with parity-time symmetry. contribution 0.92 0.68 0.09 asserted 1.00
s3 These hypersurface singularities are nonisolated degeneracies embedded entirely on exceptional surfaces, rendering the energy gaps in our systems inevitably closed at the intersections of the Brillouin zone loop and the exceptional surfaces. result 0.39 0.70 0.06 asserted 1.00
s4 Unexpectedly, such gapless systems still afford topologically protected edge states at system boundaries, challenging the conventional understanding based on band gaps. result 0.95 0.84 0.62 asserted 1.00
s5 To elucidate the existence of these edge states in the absence of a band-gap-based invariant, we propose a theoretical framework based on eigen-frame rotation and deformation that incorporates non-Bloch band theory. method 0.87 0.91 0.06 asserted 0.98
s6 Finally, we experimentally demonstrate this new form of topological edge states with nonreciprocal circuits for the first time. contribution 0.65 0.97 0.13 asserted 1.00
s7 Our work constitutes a major advance that extends topological edge states from gapped phases to gapless phases, offering new insights into topological phenomena. interpretation 0.87 0.71 0.73 asserted 1.00

What kind of paper the classifier reports this is: empirical study 0.62 · evidence from observation or experiment 0.98.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

Topologically protected edge states have been extensively studied in systems characterized by the topological invariants in band gaps (also called line gaps). In this study, we unveil a whole new form of edge states that transcends the established paradigms of band-gap topology. In contrast to the traditional stable edge states in topological insulators with specific band gaps, the one-dimensional systems we investigate are inherently gapless with the Brillouin zones being mapped to the loops encircling hypersurface singularities in a higher-dimensional space with parity-time symmetry. These hypersurface singularities are nonisolated degeneracies embedded entirely on exceptional surfaces, rendering the energy gaps in our systems inevitably closed at the intersections of the Brillouin zone loop and the exceptional surfaces. Unexpectedly, such gapless systems still afford topologically protected edge states at system boundaries, challenging the conventional understanding based on band gaps. To elucidate the existence of these edge states in the absence of a band-gap-based invariant, we propose a theoretical framework based on eigen-frame rotation and deformation that incorporates non-Bloch band theory. Finally, we experimentally demonstrate this new form of topological edge states with nonreciprocal circuits for the first time. Our work constitutes a major advance that extends topological edge states from gapped phases to gapless phases, offering new insights into topological phenomena.

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Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

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