Phononic Stiefel–Whitney Topology with Hinge Vibrational Modes in 3D Carbon Allotrope 4<sup>3</sup>T57-CA

As a fragile topological state lacking spin-orbit coupling (SOC) and possessing space-time inversion (<i>PT</i>) symmetry, the Stiefel-Whitney (SW) insulator has received much attention. Up until now, the identification of SW insulators has been extensively suggested for 2D phononic systems but has been rarely considered for 3D phononic systems. 3D carbon allotrope 4<sup>3</sup>T57-CA has the capability to achieve nontrivial phononic SW topology, which can be distinguished by a nontrivial second SW number. Moreover, 3D 4<sup>3</sup>T57-CA can host hinge vibrational modes, which are protected by <i>PT</i>.

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Publication Details

Journal
ACS Omega
Published
2024-11-04
DOI
https://doi.org/10.1021/acsomega.4c08904
Primary Topic
Topological Materials and Phenomena
Type
article
Field-Weighted Citation Impact
0.00

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article

Phononic Stiefel–Whitney Topology with Hinge Vibrational Modes in 3D Carbon Allotrope 43T57-CA

Yang Li
ACS Omega
Topological Materials and Phenomena
article

Phononic Stiefel–Whitney Topology with Hinge Vibrational Modes in 3D Carbon Allotrope 43T57-CA

Yang Li
article en

Abstract

As a fragile topological state lacking spin-orbit coupling (SOC) and possessing space-time inversion (<i>PT</i>) symmetry, the Stiefel-Whitney (SW) insulator has received much attention. Up until now, the identification of SW insulators has been extensively suggested for 2D phononic systems but has been rarely considered for 3D phononic systems. 3D carbon allotrope 4<sup>3</sup>T57-CA has the capability to achieve nontrivial phononic SW topology, which can be distinguished by a nontrivial second SW number. Moreover, 3D 4<sup>3</sup>T57-CA can host hinge vibrational modes, which are protected by <i>PT</i>.

ACS OmegaVol. 9(46)
Chongqing University (CN), Chongqing Vocational Institute of Engineering (CN)
Chongqing Municipal Education Commission
Openalex Percentile: Top 82%
Topological Materials and Phenomena
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