Universal Scaling in Intrinsic Resistivity of Two-Dimensional Metal Borophene
arXiv:1711.11186 · doi:10.1002/ange.201800087
Abstract
Two-dimensional boron sheets (borophenes) have been successfully synthesized in experiments and are expected to exhibit intriguing transport properties such as the emergence of superconductivity and Dirac Fermions. However, quantitative understanding of intrinsic electrical transport of borophene has not been achieved. Here, we report a comprehensive first-principles study on electron-phonon driven intrinsic electrical resistivity (\r{ho}) of emerging borophene structures. We find that the resistivity is highly dependent on the atomic structures and electron density of borophene. Low-temperature resistivity of borophene \r{ho} exhibits a universal scaling behavior, which increases rapidly with temperature T (\r{ho}~T^4), while \r{ho} increases linearly for a large temperature window T > 100 K. It is observed that this universal behavior of intrinsic resistivity is well described by Bloch-Grünesisen model. Different from graphene and conventional three-dimensional metals, the intrinsic resistivity of borophenes can be easily tuned by adjusting carrier densities while the Bloch-Grünesisen temperature is nearly fixed at ~100 K. Our work suggests monolayer boron can serve as an intriguing platform for realizing high-tunable two-dimensional electronic devices.
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References in corpus (9)
- Quantum ESPRESSO: a modular and open-source software project for quantum simulations of materials
- Controlling electron-phonon interactions in graphene at ultra high carrier densities
- Acoustic phonon scattering limited carrier mobility in 2D extrinsic graphene
- Dirac fermions in borophene
- Elasticity, Flexibility and Ideal Strength of Borophenes
- The electronic thermal conductivity of graphene
- Electron-Phonon Interactions and the Intrinsic Electrical Resistivity of Graphene
- Triplet Fermions and Dirac Fermions in Borophene
- Intrinsic Charge Transport in Stanene: Roles of Bucklings and Electron-Phonon Couplings