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

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

Publication Details

Journal
Figshare
Published
2024-11-04
DOI
https://doi.org/10.1021/acsomega.4c08904.s001
Primary Topic
Mycorrhizal Fungi and Plant Interactions
Type
article
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article

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

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Mycorrhizal Fungi and Plant Interactions
article

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

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Abstract

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

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Phononic Stiefel–Whitney Topology with Hinge\nVibrational Modes in 3D Carbon Allotrope 4<sup>3</sup>T57-CA · Figshare (2024) | TGRS Research Map | TGRS