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高能质子辐照对二维六方氮化硼的损伤

High-energy proton irradiation damage on two-dimensional hexagonal boron nitride.

作者信息

Lee Dongryul, Yoo Sanghyuk, Bae Jinho, Park Hyunik, Kang Keonwook, Kim Jihyun

机构信息

Department of Chemical and Biological Engineering, Korea University Seoul 02841 South Korea

Department of Mechanical Engineering, Yonsei University Seoul 03722 South Korea

出版信息

RSC Adv. 2019 Jun 11;9(32):18326-18332. doi: 10.1039/c9ra03121a. eCollection 2019 Jun 10.

DOI:10.1039/c9ra03121a
PMID:35515214
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9064770/
Abstract

The dielectric layer, which is an essential building block in electronic device circuitry, is subject to intrinsic or induced defects that limit its performance. Nano-layers of hexagonal boron nitride (h-BN) represent a promising dielectric layer in nano-electronics owing to its excellent electronic and thermal properties. In order to further analyze this technology, two-dimensional (2D) h-BN dielectric layers were exposed to high-energy proton irradiation at various proton energies and doses to intentionally introduce defective sites. A pristine h-BN capacitor showed typical degradation stages with a hard breakdown field of 10.3 MV cm, while h-BN capacitors irradiated at proton energies of 5 and 10 MeV at a dose of 1 × 10 cm showed lower hard breakdown fields of 1.6 and 8.3 MV cm, respectively. Higher leakage currents were observed under higher proton doses at 5 × 10 cm, resulting in lower breakdown fields. The degradation stages of proton-irradiated h-BN are similar to those of defective silicon dioxide. The degradation of the h-BN dielectric after proton irradiation is attributed to Frenkel defects created by the high-energy protons, as indicated by the molecular dynamics simulation. Understanding the defect-induced degradation mechanism of h-BN nano-layers can improve their reliability, paving the way to the implementation of 2D h-BN in advanced micro- and nano-electronics.

摘要

介电层是电子设备电路中的基本组成部分,会受到限制其性能的固有或诱导缺陷的影响。六方氮化硼(h-BN)纳米层由于其优异的电学和热学性能,在纳米电子学中是一种很有前景的介电层。为了进一步分析这项技术,将二维(2D)h-BN介电层在不同质子能量和剂量下暴露于高能质子辐照,以有意引入缺陷位点。一个原始的h-BN电容器显示出典型的退化阶段,其硬击穿场强为10.3 MV/cm,而在质子能量为5 MeV和10 MeV、剂量为1×10/cm下辐照的h-BN电容器,其硬击穿场强分别较低,为1.6 MV/cm和8.3 MV/cm。在质子剂量为5×10/cm时,在更高的质子剂量下观察到更高的漏电流,导致击穿场强更低。质子辐照后的h-BN的退化阶段与有缺陷的二氧化硅相似。分子动力学模拟表明,质子辐照后h-BN介电层的退化归因于高能质子产生的弗伦克尔缺陷。了解h-BN纳米层的缺陷诱导退化机制可以提高其可靠性,为在先进的微电子和纳米电子学中实现二维h-BN铺平道路。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/425872bd1f36/c9ra03121a-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/969a022a6e36/c9ra03121a-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/23127721c01a/c9ra03121a-f2.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/ded770b4e7a6/c9ra03121a-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/d47c9f2dd3be/c9ra03121a-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/425872bd1f36/c9ra03121a-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/969a022a6e36/c9ra03121a-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/23127721c01a/c9ra03121a-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/b910dc3f2585/c9ra03121a-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/ded770b4e7a6/c9ra03121a-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/d47c9f2dd3be/c9ra03121a-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0fd/9064770/425872bd1f36/c9ra03121a-f6.jpg

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