Volume 32, Issue 48 2005838
Communication

Dirac Fermion Kinetics in 3D Curved Graphene

Yoichi Tanabe

Corresponding Author

Department of Applied Science, Okayama University of Science, Okayama, 700‐0005 Japan

E‐mail: tanabe@das.ous.ac.jp, ito.yoshikazu.ga@u.tsukuba.ac.jp, mwchen@jhu.edu

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Yoshikazu Ito

Corresponding Author

Institute of Applied Physics, Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki, 305‐8573 Japan

E‐mail: tanabe@das.ous.ac.jp, ito.yoshikazu.ga@u.tsukuba.ac.jp, mwchen@jhu.edu

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Katsuaki Sugawara

Department of Physics, Graduate School of Science, Tohoku University, Sendai, 980‐8578 Japan

Advanced Institute for Materials Research, Tohoku University, Sendai, 980‐8577 Japan

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Mikito Koshino

Department of Physics, Osaka University, Osaka, 560‐0043 Japan

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Shojiro Kimura

Institute for Materials Research, Tohoku University, Sendai, 980‐8577 Japan

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Tomoya Naito

Department of Physics, Graduate School of Science, The University of Tokyo, Tokyo, 113‐0033 Japan

RIKEN Nishina Center, Wako, 351‐0198 Japan

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Isaac Johnson

Department of Materials Science and Engineering, Hopkins Extreme Materials Institute, Johns Hopkins University, Baltimore, MD, 21218 USA

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Takashi Takahashi

Advanced Institute for Materials Research, Tohoku University, Sendai, 980‐8577 Japan

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Mingwei Chen

Corresponding Author

Advanced Institute for Materials Research, Tohoku University, Sendai, 980‐8577 Japan

Department of Materials Science and Engineering, Hopkins Extreme Materials Institute, Johns Hopkins University, Baltimore, MD, 21218 USA

E‐mail: tanabe@das.ous.ac.jp, ito.yoshikazu.ga@u.tsukuba.ac.jp, mwchen@jhu.edu

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First published: 28 October 2020

Abstract

3D integration of graphene has attracted attention for realizing carbon‐based electronic devices. While the 3D integration can amplify various excellent properties of graphene, the influence of 3D curved surfaces on the fundamental physical properties of graphene has not been clarified. The electronic properties of 3D nanoporous graphene with a curvature radius down to 25–50 nm are systematically investigated and the ambipolar electronic states of Dirac fermions are essentially preserved in the 3D graphene nanoarchitectures, while the 3D curvature can effectively suppress the slope of the linear density of states of Dirac fermion near the Fermi level are demonstrated. Importantly, the 3D curvature can be utilized to tune the back‐scattering‐suppressed electrical transport of Dirac fermions and enhance both electron localization and electron–electron interaction. As a result, nanoscale curvature provides a new degree of freedom to manipulate 3D graphene electrical properties, which may pave a new way to design new 3D graphene devices with preserved 2D electronic properties and novel functionalities.

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