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首页> 外文期刊>Nanotechnology >Enhancing ultraviolet-to-visible rejection ratio by inserting an intrinsic NiO layer in p-NiO/n-Si heterojunction photodiodes
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Enhancing ultraviolet-to-visible rejection ratio by inserting an intrinsic NiO layer in p-NiO/n-Si heterojunction photodiodes

机译:通过在P-NIO / N-Si异质结光电二极管中插入内在的NIO层来提高紫外线至可见抑制比

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Conventionally, p-NiO/n-Si (p-n) heterojunction photodiodes (HPDs) exhibit a larger visible response than the ultraviolet response due to the thick Si substrate; hence, it is used as a broadband photodetector with a poor ultraviolet (UV)-to-visible rejection ratio. Herein, an intrinsic NiO (i-NiO) layer is inserted between the p-NiO and the n-Si substrate to fabricate p-NiO/i-NiO/n-Si (p-i-n) HPDs, significantly suppressing leakage current and visible response. Compared with the conventional p-n HPDs, the insertion of the i-NiO layer significantly reduces leakage current by approximately 241 times and enhances the rectification ratio from 13.8 to 3228 for the p-n and p-i-n HPDs. The insertion of an i-NiO layer not only increases the UV-response but also suppresses the visible response. These issues enhance the UV-to-visible rejection ratio from 72.2 in p-n HPDs to 915.3 in p-i-n HPDs. The p-NiO reveals a poorer crystalline structure than the i-NiO film because the Ag dopants accumulate at the grain boundary and inhibit crystalline growth. The Ag diffusion in the Si substrate causes defect states within the Si bandgap, whereas it is retarded by the i-NiO layer in the p-i-n HPDs. The poor crystallinity in the p-NiO and defect states within the Si bandgap contributes to a high leakage current and visible response in p-n HPDs. The p-i-n HPDs demonstrate a higher UV-response due to absorption by the i-NiO layer. Because visible light cannot be absorbed by the i-NiO layer, visible response is suppressed in p-i-n HPDs.
机译:通常,P-NiO / N-Si(P-N)异质结光电二极管(HPD)表现出比厚Si衬底引起的紫外线响应更大的可见响应;因此,它用作具有差的紫外线(UV)-To可见抑制比的宽带光电探测器。在此,在P-NIO和N-Si底物之间插入本征NiO(I-NIO)层以制造P-NiO / I-NiO / N-Si(P-I-N)HPD,显着抑制漏电流和可见响应。与传统的P-N HPD相比,I-NIO层的插入显着降低了漏电流约241次,并增强了P-N和P-I-N HPD的13.8至3228的整流比。 I-NIO层的插入不仅增加了UV响应,而且还抑制了可见响应。这些问题提高了P-I-N HPDS中的72.2中的紫外线可见抑制比在P-I-N HPDS中的915.3。 P-NIO显示比I-NiO膜更差的结晶结构,因为Ag掺杂剂在晶界积聚并抑制结晶生长。 Si衬底中的Ag扩散导致Si带隙内的缺陷状态,而它被P-I-N HPD中的I-NiO层延迟。在Si带隙内的p-nio和缺陷状态下的差的结晶度有助于p-n Hpds的高漏电流和可见响应。 P-I-N HPDS由于I-NIO层的吸收而证明了更高的UV响应。因为可见光不能被I-NIO层吸收,所以在P-I-N HPD中抑制了可见响应。

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