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半导体中栅极可调的接触诱导费米能级移动。

Gate-tunable contact-induced Fermi-level shift in semimetal.

机构信息

State Key Laboratory of Low-Dimensional Quantum Physics, Department of Physics and Tsinghua-Foxconn Nanotechnology Research Center, Tsinghua University, Beijing 100084, China.

Beijing Innovation Center for Future Chips, Tsinghua University, Beijing 100084, China.

出版信息

Proc Natl Acad Sci U S A. 2022 Apr 26;119(17):e2119016119. doi: 10.1073/pnas.2119016119. Epub 2022 Apr 22.

DOI:10.1073/pnas.2119016119
PMID:35452312
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9169931/
Abstract

Low-dimensional semimetal–semiconductor (Sm-S) van der Waals (vdW) heterostructures have shown their potentials in nanoelectronics and nano-optoelectronics recently. It is an important scientific issue to study the interfacial charge transfer as well as the corresponding Fermi-level shift in Sm-S systems. Here we investigated the gate-tunable contact-induced Fermi-level shift (CIFS) behavior in a semimetal single-walled carbon nanotube (SWCNT) that formed a heterojunction with a transition-metal dichalcogenide (TMD) flake. A resistivity comparison methodology and a Fermi-level catch-up model have been developed to measure and analyze the CIFS, whose value is determined by the resistivity difference between the naked SWCNT segment and the segment in contact with the TMD. Moreover, the relative Fermi-level positions of SWCNT and two-dimensional (2D) semiconductors can be efficiently reflected by the gate-tunable resistivity difference. The work function change of the semimetal, as a result of CIFS, will naturally introduce a modified form of the Schottky–Mott rule, so that a modified Schottky barrier height can be obtained for the Sm-S junction. The methodology and physical model should be useful for low-dimensional reconfigurable nanodevices based on Sm-S building blocks.

摘要

低维半导体-金属(Sm-S)范德华(vdW)异质结在纳电子学和纳光电学领域显示出了巨大的潜力。研究 Sm-S 体系中的界面电荷转移以及相应的费米能级移动是一个重要的科学问题。在这里,我们研究了由过渡金属二卤化物(TMD)薄片构成的异质结的半导体单壁碳纳米管(SWCNT)中栅极可调的接触诱导费米能级移动(CIFS)行为。我们开发了一种电阻率比较方法和费米能级追赶模型来测量和分析 CIFS,其值由与 TMD 接触的裸露 SWCNT 段和与 TMD 接触的 SWCNT 段之间的电阻率差异决定。此外,SWCNT 和二维(2D)半导体的相对费米能级位置可以通过栅极可调的电阻率差异有效地反映出来。由于 CIFS,金属的功函数变化将自然引入肖特基-莫特规则的修正形式,从而可以获得 Sm-S 结的修正肖特基势垒高度。该方法和物理模型应该对基于 Sm-S 构建块的低维可重构纳米器件有用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/d83398a50aa7/pnas.2119016119fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/92feeaa75f33/pnas.2119016119fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/d32c5f901f43/pnas.2119016119fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/14843c5eefe0/pnas.2119016119fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/1904d81cade0/pnas.2119016119fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/d83398a50aa7/pnas.2119016119fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/92feeaa75f33/pnas.2119016119fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/d32c5f901f43/pnas.2119016119fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/14843c5eefe0/pnas.2119016119fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/1904d81cade0/pnas.2119016119fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5e2e/9169931/d83398a50aa7/pnas.2119016119fig05.jpg

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