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缺陷诱导的发光猝灭与硅纳米晶体中掺入的磷的电荷载流子产生随尺寸的变化关系。

Defect-Induced Luminescence Quenching vs. Charge Carrier Generation of Phosphorus Incorporated in Silicon Nanocrystals as Function of Size.

作者信息

Hiller Daniel, López-Vidrier Julian, Gutsch Sebastian, Zacharias Margit, Nomoto Keita, König Dirk

机构信息

Laboratory for Nanotechnology, Dept. of Microsystems Engineering (IMTEK), University of Freiburg, Freiburg, Germany.

School of Photovoltaic and Renewable Energy Engineering (SPREE), University of New South Wales (UNSW), Sydney, Australia.

出版信息

Sci Rep. 2017 Apr 13;7(1):863. doi: 10.1038/s41598-017-01001-1.

DOI:10.1038/s41598-017-01001-1
PMID:28408757
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5429832/
Abstract

Phosphorus doping of silicon nanostructures is a non-trivial task due to problems with confinement, self-purification and statistics of small numbers. Although P-atoms incorporated in Si nanostructures influence their optical and electrical properties, the existence of free majority carriers, as required to control electronic properties, is controversial. Here, we correlate structural, optical and electrical results of size-controlled, P-incorporating Si nanocrystals with simulation data to address the role of interstitial and substitutional P-atoms. Whereas atom probe tomography proves that P-incorporation scales with nanocrystal size, luminescence spectra indicate that even nanocrystals with several P-atoms still emit light. Current-voltage measurements demonstrate that majority carriers must be generated by field emission to overcome the P-ionization energies of 110-260 meV. In absence of electrical fields at room temperature, no significant free carrier densities are present, which disproves the concept of luminescence quenching via Auger recombination. Instead, we propose non-radiative recombination via interstitial-P induced states as quenching mechanism. Since only substitutional-P provides occupied states near the Si conduction band, we use the electrically measured carrier density to derive formation energies of ~400 meV for P-atoms on Si nanocrystal lattice sites. Based on these results we conclude that ultrasmall Si nanovolumes cannot be efficiently P-doped.

摘要

由于存在限制、自净化和少量统计等问题,对硅纳米结构进行磷掺杂并非易事。尽管掺入硅纳米结构中的磷原子会影响其光学和电学性质,但控制电子性质所需的自由多数载流子的存在仍存在争议。在这里,我们将尺寸可控、掺磷的硅纳米晶体的结构、光学和电学结果与模拟数据相关联,以探讨间隙和替代磷原子的作用。原子探针断层扫描证明磷的掺入量与纳米晶体尺寸成正比,而发光光谱表明,即使含有几个磷原子的纳米晶体仍能发光。电流-电压测量表明,多数载流子必须通过场发射产生,以克服110-260 meV的磷电离能。在室温下没有电场的情况下,不存在明显的自由载流子密度,这反驳了通过俄歇复合实现发光猝灭的概念。相反,我们提出通过间隙磷诱导态的非辐射复合作为猝灭机制。由于只有替代磷在硅导带附近提供占据态,我们利用电学测量的载流子密度得出硅纳米晶体晶格位置上磷原子的形成能约为400 meV。基于这些结果,我们得出结论,超小的硅纳米体积不能有效地进行磷掺杂。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/858b328a6bcd/41598_2017_1001_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/cf4e5ab394b2/41598_2017_1001_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/f976e0052286/41598_2017_1001_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/6a6ad2400204/41598_2017_1001_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/0d86d97b00ca/41598_2017_1001_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/63a88f8f323d/41598_2017_1001_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/858b328a6bcd/41598_2017_1001_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/cf4e5ab394b2/41598_2017_1001_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/f976e0052286/41598_2017_1001_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/6a6ad2400204/41598_2017_1001_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/0d86d97b00ca/41598_2017_1001_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/63a88f8f323d/41598_2017_1001_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d41/5429832/858b328a6bcd/41598_2017_1001_Fig6_HTML.jpg

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