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用氢氧化铵处理以实现水热法制备的镓掺杂n-ZnO/p-Si异质结构特性的最佳形态权衡。

NH₄OH Treatment for an Optimum Morphological Trade-off to Hydrothermal Ga-Doped n-ZnO/p-Si Heterostructure Characteristics.

作者信息

Rana Abu Ul Hassan Sarwar, Kim Hyun-Seok

机构信息

Division of Electronics and Electrical Engineering, Dongguk University-Seoul, Seoul 04620, Korea.

出版信息

Materials (Basel). 2017 Dec 27;11(1):37. doi: 10.3390/ma11010037.

DOI:10.3390/ma11010037
PMID:29280963
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5793535/
Abstract

Previous studies on Ga-doped ZnO nanorods (GZRs) have failed to address the change in GZR morphology with increased doping concentration. The morphology-change affects the GZR surface-to-volume ratio and the real essence of doping is not exploited for heterostructure optoelectronic characteristics. We present NH₄OH treatment to provide an optimum morphological trade-off to n-GZR/p-Si heterostructure characteristics. The GZRs were grown via one of the most eminent and facile hydrothermal method with an increase in Ga concentration from 1% to 5%. The supplementary OH ion concentration was effectively controlled by the addition of an optimum amount of NH₄OH to synchronize GZR aspect and surface-to-volume ratio. Hence, the probed results show only the effects of Ga-doping, rather than the changed morphology, on the optoelectronic characteristics of n-GZR/p-Si heterostructures. The doped nanostructures were characterized by scanning electron microscopy, energy dispersive X-ray spectroscopy, X-ray diffraction, photoluminescence, Hall-effect measurement, and Keithley 2410 measurement systems. GZRs had identical morphology and dimensions with a typical wurtzite phase. As the GZR carrier concentration increased, the PL response showed a blue shift because of Burstein-Moss effect. Also, the heterostructure current levels increased linearly with doping concentration. We believe that the presented GZRs with optimized morphology have great potential for field-effect transistors, light-emitting diodes, ultraviolet sensors, and laser diodes.

摘要

先前对镓掺杂氧化锌纳米棒(GZRs)的研究未能解决随着掺杂浓度增加 GZR 形态的变化问题。形态变化会影响 GZR 的表面体积比,并且未充分利用掺杂的真正本质来研究异质结构的光电特性。我们提出用氢氧化铵处理,以在 n-GZR/p-Si 异质结构特性方面实现最佳的形态权衡。GZRs 通过最著名且简便的水热法生长,镓浓度从 1%增加到 5%。通过添加适量的氢氧化铵有效控制额外的氢氧根离子浓度,以同步 GZR 的长径比和表面体积比。因此,所探究的结果表明,在 n-GZR/p-Si 异质结构的光电特性中,仅存在镓掺杂的影响,而非形态变化的影响。通过扫描电子显微镜、能量色散 X 射线光谱、X 射线衍射、光致发光、霍尔效应测量和 Keithley 2410 测量系统对掺杂的纳米结构进行了表征。GZRs 具有相同的形态和尺寸,呈典型的纤锌矿相。随着 GZR 载流子浓度的增加,由于伯斯坦 - 莫斯效应,光致发光响应出现蓝移。此外,异质结构的电流水平随掺杂浓度线性增加。我们认为,所呈现的具有优化形态的 GZRs 在场效应晶体管、发光二极管、紫外传感器和激光二极管方面具有巨大潜力。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/c39e253a0fcf/materials-11-00037-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/c46e4aee6bd4/materials-11-00037-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/61566d972c9d/materials-11-00037-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/0971836a9bc2/materials-11-00037-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/090acad7fbcc/materials-11-00037-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/28b6467cb38b/materials-11-00037-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/6d2f1ae1c4ec/materials-11-00037-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/1e4926b1740a/materials-11-00037-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/0afde94706db/materials-11-00037-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/c39e253a0fcf/materials-11-00037-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/c46e4aee6bd4/materials-11-00037-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/61566d972c9d/materials-11-00037-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/0971836a9bc2/materials-11-00037-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/090acad7fbcc/materials-11-00037-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/28b6467cb38b/materials-11-00037-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/6d2f1ae1c4ec/materials-11-00037-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/1e4926b1740a/materials-11-00037-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/0afde94706db/materials-11-00037-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e5f3/5793535/c39e253a0fcf/materials-11-00037-g009.jpg

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