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半导体碳纳米管中衬底诱导的带隙重整化。

Substrate-induced band gap renormalization in semiconducting carbon nanotubes.

机构信息

Department of Physics, Applied Physics, and Astronomy, Rensselaer Polytechnic Institute, 110 8th Street, Troy, NY 12180.

Computational Center for Nanotechnology Innovation, Troy, NY 12180, USA.

出版信息

Sci Rep. 2014 Jan 9;4:3609. doi: 10.1038/srep03609.

Abstract

The quasiparticle band gaps of semiconducting carbon nanotubes (CNTs) supported on a weakly-interacting hexagonal boron nitride (h-BN) substrate are computed using density functional theory and the GW Approximation. We find that the direct band gaps of the (7,0), (8,0) and (10,0) carbon nanotubes are renormalized to smaller values in the presence of the dielectric h-BN substrate. The decrease in the band gap is the result of a polarization-induced screening effect, which alters the correlation energy of the frontier CNT orbitals and stabilizes valence band maximum and conduction band minimum. The value of the band gap renormalization is on the order of 0.25 to 0.5 eV in each case. Accounting for polarization-induced band gap changes is crucial in comparing computed values with experiment, since nanotubes are almost always grown on substrates.

摘要

使用密度泛函理论和 GW 近似,我们计算了弱相互作用六方氮化硼(h-BN)衬底上支撑的半导体碳纳米管(CNT)的准粒子能带隙。我们发现,在存在介电 h-BN 衬底的情况下,(7,0)、(8,0)和(10,0)碳纳米管的直接带隙被重新归一化为较小的值。带隙的减小是极化诱导屏蔽效应的结果,它改变了前沿 CNT 轨道的关联能,并稳定了价带最大值和导带最小值。在每种情况下,带隙重整化的值约为 0.25 到 0.5 eV。考虑极化诱导的带隙变化对于将计算值与实验进行比较至关重要,因为纳米管几乎总是在衬底上生长。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/68c5/3885876/c6dc2535a860/srep03609-f1.jpg

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