First-principles calculations on the intrinsic resistivity of borophene: anisotropy and temperature dependence. Issue 4 (9th January 2019)

• Record Type: Journal Article
• Authors: Liu, Zhe; Zhu, Mingfeng; Zheng, Yisong
• Is Part Of: Journal of materials chemistry. Volume 7:Issue 4(2019)
• Page Start: 986
• Page End: 997
• Publication Date: 2019-01-09
• Subjects: Materials -- Periodicals; Chemistry, Analytic -- Periodicals; Optical materials -- Research -- Periodicals; Electronics -- Materials -- Research -- Periodicals; 543.0284
• DOI: 10.1039/c8tc05269g
• Languages: English
• ISSNs: 2050-7526

Abstract

Abstract : Temperature dependence and anisotropy of the intrinsic resistivity of β 12 and χ 3 borophene. Abstract : The intrinsic resistivity arising from electron–phonon scattering is an important property of metals, especially at room temperature. Borophene, a kind of successfully synthesized two-dimensional (2D) boron sheet, exhibits metallic electronic transport behavior. In this paper, we report first-principles calculations on the intrinsic resistivity of two borophene allotropes, called β 12 and χ 3 . At first, we find that the intrinsic resistivity of the two structures shows non-trivial anisotropy which amounts to at least 28%. In addition, our calculations indicate that the intrinsic resistivity of β 12 and χ 3 are both proportional to temperature in the high-temperature region (>160 K). However, in the low-temperature region (<70 K), the T 4 -law of the intrinsic resistivity predicted by the Bloch–Grüneisen theory for 2D metals holds true for β 12 but breaks down for χ 3 . Based on a detailed analysis, we find that the two borophenes have complicated Fermi surfaces with multiple branches. Optical phonon modes in β 12 and the Umklapp process in χ 3 play non-trivial roles in the low-temperature region. All of these factors influencing the intrinsic resistivity of borophene are beyond the simplifications adopted in the Bloch–Grüneisen theory. Therefore, we conclude that the Bloch–Grüneisen theory is inapplicable to explain the temperature dependence of the intrinsic resistivity of β 12 and χ 3, two experimentally available 2D metals.