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具有极高空穴有效迁移率和超过六个数量级的导通电流/截止电流的氧化锡纳米片晶体管。

SnO Nanosheet Transistor with Remarkably High Hole Effective Mobility and More than Six Orders of Magnitude On-Current/Off-Current.

作者信息

Chen Kuan-Chieh, Wu Jiancheng, Pooja Pheiroijam, Chin Albert

机构信息

Department of Electronics Engineering, National Yang Ming Chiao Tung University, Hsinchu 300, Taiwan.

出版信息

Nanomaterials (Basel). 2025 Apr 23;15(9):640. doi: 10.3390/nano15090640.

DOI:10.3390/nano15090640
PMID:40358257
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12074316/
Abstract

Using novel SiO surface passivation and ultraviolet (UV) light anneal, a 12 nm thick SnO p-type FET (pFET) shows hole effective mobilities (µ) of more than 100 cm/V·s and 31.1 cm/V·s at hole densities (Q) of 1 × 10 and 5 × 10 cm, respectively. To further improve the on-current/off-current (I/I), an ultra-thin 7 nm thick SnO nanosheet pFET shows a record-breaking I/I of 6.9 × 10 and remarkable µ values of ~70 cm/V·s and 20.7 cm/V·s at Q of 1 × 10 cm and 5 × 10 cm, respectively. This is the first report of an oxide semiconductor transistor achieving a hole effective mobility µ that reaches 20% of that in single-crystal Si pFETs at an ultra-thin body thickness of 7 nm. In sharp contrast, the control SnO nanosheet pFET without surface passivation or UV anneal exhibits a small I/I of 1.8 × 10 and a µ of only 6.1 cm/V·s at 5 × 10 cm Q. The enhanced SnO pFET performance is attributed to reduced defects and improved quality in the SnO channel, as confirmed by decreased charges related to sub-threshold swing (SS) and threshold voltage (Vth) shift. Such a large improvement is further supported by the increased Sn after passivation and UV anneal, as evidenced by X-ray photoelectron spectroscopy (XPS) analysis. The I/I ratio exceeding six orders of magnitude, remarkably high hole µ, and excellent two-month stability demonstrate that this pFET is a strong candidate for integration with SnON nFETs in next-generation ultra-high-definition displays and monolithic three-dimensional integrated circuits (3D ICs).

摘要

通过采用新型的SiO表面钝化和紫外(UV)光退火工艺,一个12纳米厚的SnO p型场效应晶体管(pFET)在空穴密度(Q)分别为1×10和5×10厘米时,展现出超过100厘米²/伏·秒和31.1厘米²/伏·秒的空穴有效迁移率(µ)。为了进一步提高开电流/关电流(Ion/Ioff),一个超薄的7纳米厚的SnO纳米片pFET在Q为1×10厘米和5×10厘米时,分别展现出破纪录的6.9×10的Ion/Ioff以及约70厘米²/伏·秒和20.7厘米²/伏·秒的显著µ值。这是关于氧化物半导体晶体管的首次报道,该晶体管在7纳米的超薄体厚度下实现了空穴有效迁移率µ达到单晶硅pFET中迁移率的20%。形成鲜明对比的是,未进行表面钝化或UV退火的对照SnO纳米片pFET在5×10厘米的Q时,展现出1.8×10的小Ion/Ioff和仅6.1厘米²/伏·秒的µ。SnO pFET性能的增强归因于SnO沟道中缺陷的减少和质量的改善,这通过与亚阈值摆幅(SS)和阈值电压(Vth)偏移相关的电荷减少得到证实。钝化和UV退火后Sn含量的增加进一步支持了如此大的性能提升,这由X射线光电子能谱(XPS)分析所证明。超过六个数量级的Ion/Ioff比、非常高的空穴µ以及出色的两个月稳定性表明,这种pFET是下一代超高分辨率显示器和单片三维集成电路(3D IC)中与SnON nFET集成的有力候选者。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/91ff61e7b040/nanomaterials-15-00640-g012.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/189fce392017/nanomaterials-15-00640-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/4768aa8cb058/nanomaterials-15-00640-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/c2b9b9395fe5/nanomaterials-15-00640-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/cb53548092e1/nanomaterials-15-00640-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/6a49c9800c85/nanomaterials-15-00640-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/4c8e34fb8979/nanomaterials-15-00640-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/defae2b6c36b/nanomaterials-15-00640-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/91ff61e7b040/nanomaterials-15-00640-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/b90785686f6b/nanomaterials-15-00640-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/18e157c9f57e/nanomaterials-15-00640-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/56539a13c35d/nanomaterials-15-00640-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/6094e5a47944/nanomaterials-15-00640-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/189fce392017/nanomaterials-15-00640-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/4768aa8cb058/nanomaterials-15-00640-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/c2b9b9395fe5/nanomaterials-15-00640-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/cb53548092e1/nanomaterials-15-00640-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/6a49c9800c85/nanomaterials-15-00640-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/4c8e34fb8979/nanomaterials-15-00640-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/defae2b6c36b/nanomaterials-15-00640-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/79e3/12074316/91ff61e7b040/nanomaterials-15-00640-g012.jpg

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