4.5 Article

Evolution of Weyl-like semi-metallicity in an all-sp2 carbon allotrope

Journal

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.jpcs.2023.111229

Keywords

Topological phase transition; All-sp2 carbon; Semi-metallicity; Symmetry protection mechanism

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Using first-principles calculations, we have designed a stable 3D all-sp2 carbon allotrope called oC32, which consists of dehydrogenized helical polyethylenes and dehydrogenized ethylenes. The absence of spin-orbit coupling leads to the existence of a Weyl-like loop in oC32, protected by time-reversal, spatial inversion, and mirror reflection symmetries. By breaking the spatial symmetries of oC32, topological phase transitions occur from the Weyl-like loop state to Weyl-like point states, which can be attributed to 2D sheets embedded in oC32. Carbon materials exhibit rich topological states and phase transitions due to their flexible bonding and negligible spin-orbit interaction.
Based on first-principles calculations, we design a stable 3D all-sp2 carbon allotrope by assembling the dehy-drogenized helical polyethylenes and dehydrogenized ethylenes. It possesses 32 carbon atoms in its unit cell with orthorhombic symmetry, thus termed oC32. In the absence of spin-orbit-coupling (SOC), oC32 possesses a Weyl-like loop protected by the coexistence of time-reversal, spatial inversion, and mirror reflection symmetries. By displacing the carbon atoms of dehydrogenized ethylenes, the spatial symmetries of oC32 are broken and to-pological phase transitions occur from the Weyl-like loop state to Weyl-like point states. To probe the origin of the Weyl-like points, we further examine the electronic properties of a 2D sheet composed of the dehydrogenized helical polyethylenes embedded in oC32 since the charge near the Fermi level is regularly distributed around these 2D sheets. We find that the Weyl-like points also appear in these 2D sheets, indicating that the Weyl-like points in the symmetry-broken oC32 come from the 2D sheets embedded in oC32. Our work demonstrates that carbon materials can exhibit rich topological states and topological phase transitions due to the flexible bonding and negligible spin-orbital interaction of carbon atom.

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