Field-effect transistors and photodetectors based on solution-synthesized nanowires

Amol Singh, A. Khandelwal, X. Li, H. Xing, Masaru Kuno, D. Jena
{"title":"Field-effect transistors and photodetectors based on solution-synthesized nanowires","authors":"Amol Singh, A. Khandelwal, X. Li, H. Xing, Masaru Kuno, D. Jena","doi":"10.1109/DRC.2006.305121","DOIUrl":null,"url":null,"abstract":"submitted to DRC 2006 Field-effect transistors and photodetectors based on solutionsynthesized nanowires A. Singh, A. Khandelwal, X. Li, H. Xing, M. Kuno, D. Jena University of Notre Dame, Notre Dame, IN 46556 Phone: 574 631 8835, Fax: 574 631 4393, email: djenagnd.edu Various semiconductor nanostructures, including nanotubes and nanowires have been grown and studied recently. The primary growth technique has been chemical vapor deposition (CVD)-based, such as the rather popular vaporliquid-solid (VLS) technique. [1] Growth techniques utilizing solution-based synthesis, on the other hand, have a number of advantages over the CVD technique such as low cost, scaling of production, ability to passivate the semiconductor surface chemically during growth, and the ease of transfer to any substrate. One such synthetic method is the solution-liquid-solid (SLS) technique, which has been used by various groups to produce colloidal quantum dots or nanocrystals.[2] Rudimentary photodetectors have been demonstrated using closed-packed \"solids\" of the SLS-grown nanocrystals. Though photon absorption and electron-hole pair generation in nanocrystals is efficient, the extraction of carriers is difficult, involving hopping transport between the dots before being collected by the electrodes. In this work, we demonstrate photodetectors based on CdSe nanowire networks, or \"quantum-wire solids\". Nanowires allow band-transport along their axes, therefore potentially offering a drastic improvement over nanocrystals for the efficient collection of optically generated carriers. To evaluate the transport properties of the nanowires, we have fabricated field-effect transistors using both single nanowires and networks of nanowires as channels on SiO2/Si substrates with back gates. For single nanowire FETs, focused ion beam has been employed to define Pt source-drain contacts. Typical nanowires diameters are 10nms, and lengths vary from 1-10 microns. For multiple nanowire channels, we have used ac dielectrophoretic alignment for precise placement of the nanowires between the source-drain contacts (Figure 1, right).[3] The nanowires FETs thus fabricated require a negative gate bias for pinch-off indicating that the wires are n-type, and drain-source current on/off ratios of 105 are observed for FETs with dense nanowires network channels, as opposed to -10 for single nanowires FETs (Figure 2, right). The temperature-dependence of the source-drain current (Fig 3, left) indicates that the charge transport is dominated by thermally generated carriers in the dark. Metal-semiconductor-metal photodetector devices are then fabricated using conventional optical lithography and metal deposition. The photodetectors are found to have very low dark currents (10 nA at 5 V), indicating very few free carriers in the nanowires at room temperature. The spectroscopic photoresponse of these photodetectors is measured using a xenon lamp coupled with a monochromator, and a lock-in amplifier in a photon energy range of 1.4 3.5 eV. We observe a sharp turn-on in the photocurrent, at 1.80 eV, near the absorption edge of the nanowires measured independently using an UV-Vis spectrophotometer (Figure 3, center). The photoresponse is estimated to be higher than 50 mA/W at a bias of 5 V at 550 nm (2.25 eV) illumination. With increasing photon energy, the responsivity of the NW-based photodetectors shows a very slow decrease, 18% drop at 3.4 eV compared to that at 2.25 eV. This is in sharp contrast to traditional photodetectors, where the photoresponse decays rapidly with increasing photon energy. The photoresponse, and the resultant quantum efficiency can be enhanced for particular wavelengths by a cavity effect by tuning the thickness of the underlying SiO2 layer and using multiple reflections from the SiO2/Si interface, as demonstrated in Figure 3 (right). In conclusion, we have demonstrated that solution-synthesized semiconductor nanowires can be used as channels in traditional FET structures, and their high optical absorption and high quantum efficiencies can be exploited for fabrication of photodetectors. With solution synthesized narrow bandgap semiconductor (PbS, PbSe) nanowires, the photodetector spectral range can be extended into the IR regime, and can be transferred to flexible substrates in the future. [4] [1] Y. Huang, Duan X., Y. Cui, L. Lauhon, K.-H. Kim, and C. Lieber, Nature (London) 294, 1313 (2001). [2] C. B. Murray, C. R. Kagan, and M. G. Bawendi, Annu. Rev. Mater. Sci. 30, 545 (2000). [3] R. Zhou, H.-C. Chang, V. Protansenko, M. Kuno, A. Singh, and D. Jena, unpublished (2006). [4] H. Petersson, J. Tragardh, A. I. Persson, L. Landin, D. Hessman, and L. Samuelson, Nano Letters 6, 229 (2006). 0-7803-9749-5/06/$20.00 ©2006 IEEE 67 Abstract submitted to DRC 2006submitted to DRC 2006 Fig. 1: Solution-synthesized CdSe nanowires (left, center), and their ac electric-field assisted dielectrophoretic alignment between contact pads in solution (right).","PeriodicalId":259981,"journal":{"name":"2006 64th Device Research Conference","volume":"9 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2006-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2006 64th Device Research Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DRC.2006.305121","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

submitted to DRC 2006 Field-effect transistors and photodetectors based on solutionsynthesized nanowires A. Singh, A. Khandelwal, X. Li, H. Xing, M. Kuno, D. Jena University of Notre Dame, Notre Dame, IN 46556 Phone: 574 631 8835, Fax: 574 631 4393, email: djenagnd.edu Various semiconductor nanostructures, including nanotubes and nanowires have been grown and studied recently. The primary growth technique has been chemical vapor deposition (CVD)-based, such as the rather popular vaporliquid-solid (VLS) technique. [1] Growth techniques utilizing solution-based synthesis, on the other hand, have a number of advantages over the CVD technique such as low cost, scaling of production, ability to passivate the semiconductor surface chemically during growth, and the ease of transfer to any substrate. One such synthetic method is the solution-liquid-solid (SLS) technique, which has been used by various groups to produce colloidal quantum dots or nanocrystals.[2] Rudimentary photodetectors have been demonstrated using closed-packed "solids" of the SLS-grown nanocrystals. Though photon absorption and electron-hole pair generation in nanocrystals is efficient, the extraction of carriers is difficult, involving hopping transport between the dots before being collected by the electrodes. In this work, we demonstrate photodetectors based on CdSe nanowire networks, or "quantum-wire solids". Nanowires allow band-transport along their axes, therefore potentially offering a drastic improvement over nanocrystals for the efficient collection of optically generated carriers. To evaluate the transport properties of the nanowires, we have fabricated field-effect transistors using both single nanowires and networks of nanowires as channels on SiO2/Si substrates with back gates. For single nanowire FETs, focused ion beam has been employed to define Pt source-drain contacts. Typical nanowires diameters are 10nms, and lengths vary from 1-10 microns. For multiple nanowire channels, we have used ac dielectrophoretic alignment for precise placement of the nanowires between the source-drain contacts (Figure 1, right).[3] The nanowires FETs thus fabricated require a negative gate bias for pinch-off indicating that the wires are n-type, and drain-source current on/off ratios of 105 are observed for FETs with dense nanowires network channels, as opposed to -10 for single nanowires FETs (Figure 2, right). The temperature-dependence of the source-drain current (Fig 3, left) indicates that the charge transport is dominated by thermally generated carriers in the dark. Metal-semiconductor-metal photodetector devices are then fabricated using conventional optical lithography and metal deposition. The photodetectors are found to have very low dark currents (10 nA at 5 V), indicating very few free carriers in the nanowires at room temperature. The spectroscopic photoresponse of these photodetectors is measured using a xenon lamp coupled with a monochromator, and a lock-in amplifier in a photon energy range of 1.4 3.5 eV. We observe a sharp turn-on in the photocurrent, at 1.80 eV, near the absorption edge of the nanowires measured independently using an UV-Vis spectrophotometer (Figure 3, center). The photoresponse is estimated to be higher than 50 mA/W at a bias of 5 V at 550 nm (2.25 eV) illumination. With increasing photon energy, the responsivity of the NW-based photodetectors shows a very slow decrease, 18% drop at 3.4 eV compared to that at 2.25 eV. This is in sharp contrast to traditional photodetectors, where the photoresponse decays rapidly with increasing photon energy. The photoresponse, and the resultant quantum efficiency can be enhanced for particular wavelengths by a cavity effect by tuning the thickness of the underlying SiO2 layer and using multiple reflections from the SiO2/Si interface, as demonstrated in Figure 3 (right). In conclusion, we have demonstrated that solution-synthesized semiconductor nanowires can be used as channels in traditional FET structures, and their high optical absorption and high quantum efficiencies can be exploited for fabrication of photodetectors. With solution synthesized narrow bandgap semiconductor (PbS, PbSe) nanowires, the photodetector spectral range can be extended into the IR regime, and can be transferred to flexible substrates in the future. [4] [1] Y. Huang, Duan X., Y. Cui, L. Lauhon, K.-H. Kim, and C. Lieber, Nature (London) 294, 1313 (2001). [2] C. B. Murray, C. R. Kagan, and M. G. Bawendi, Annu. Rev. Mater. Sci. 30, 545 (2000). [3] R. Zhou, H.-C. Chang, V. Protansenko, M. Kuno, A. Singh, and D. Jena, unpublished (2006). [4] H. Petersson, J. Tragardh, A. I. Persson, L. Landin, D. Hessman, and L. Samuelson, Nano Letters 6, 229 (2006). 0-7803-9749-5/06/$20.00 ©2006 IEEE 67 Abstract submitted to DRC 2006submitted to DRC 2006 Fig. 1: Solution-synthesized CdSe nanowires (left, center), and their ac electric-field assisted dielectrophoretic alignment between contact pads in solution (right).
基于溶液合成纳米线的场效应晶体管和光电探测器
A. Singh, A. Khandelwal, X. Li,邢宏,M. Kuno, D. jenagnd.e nna University of Notre Dame, IN 46556电话:574 631 8835,传真:574 631 4393,电子邮件:djenagnd.edu近年来各种半导体纳米结构,包括纳米管和纳米线的生长和研究。主要的生长技术是以化学气相沉积(CVD)为基础的,例如相当流行的汽液固相沉积(VLS)技术。[1]另一方面,利用溶液合成的生长技术与CVD技术相比具有许多优势,例如低成本,生产规模,在生长过程中化学钝化半导体表面的能力,以及易于转移到任何衬底上。其中一种合成方法是溶液-液-固(SLS)技术,该技术已被各种团体用于生产胶体量子点或纳米晶体。[2]使用sls生长的纳米晶体的封闭“固体”,已经证明了基本的光电探测器。虽然纳米晶体中的光子吸收和电子空穴对的产生是有效的,但载流子的提取是困难的,在被电极收集之前涉及到点之间的跳变输运。在这项工作中,我们展示了基于CdSe纳米线网络或“量子线固体”的光电探测器。纳米线允许沿其轴带传输,因此在有效收集光学生成的载流子方面,可能比纳米晶体提供了巨大的改进。为了评估纳米线的输运特性,我们在带有后门的SiO2/Si衬底上制备了单纳米线和纳米线网络作为通道的场效应晶体管。对于单纳米线场效应管,聚焦离子束被用来定义铂源漏触点。典型的纳米线直径为10nm,长度为1-10微米。对于多个纳米线通道,我们使用交流介电泳对齐来精确放置源漏触点之间的纳米线(图1,右)。[3]这样制造的纳米线场效应管需要负栅极偏置用于掐断,这表明线是n型的,并且对于具有密集纳米线网络通道的场效应管,观察到漏源电流的通断比为105,而对于单纳米线场效应管,则为-10(图2,右)。源漏电流的温度依赖性(图3,左)表明,在黑暗中,电荷输运主要由热产生的载流子控制。然后利用传统的光学光刻和金属沉积技术制造金属-半导体-金属光电探测器装置。发现光电探测器具有非常低的暗电流(5v时10na),表明室温下纳米线中的自由载流子很少。在光子能量范围为1.4 - 3.5 eV的情况下,利用氙灯、单色器和锁相放大器测量了这些光电探测器的光谱光响应。我们观察到光电流在1.80 eV时急剧开启,在纳米线的吸收边缘附近,使用紫外可见分光光度计独立测量(图3,中心)。估计在550nm (2.25 eV)照明下,在5v偏置下的光响应高于50ma /W。随着光子能量的增加,nw基光电探测器的响应率呈缓慢下降趋势,在3.4 eV时比在2.25 eV时下降18%。这与传统的光电探测器形成鲜明对比,传统的光电探测器的光响应随着光子能量的增加而迅速衰减。光响应和由此产生的量子效率可以通过调整底层SiO2层的厚度和使用来自SiO2/Si界面的多次反射的空腔效应来增强特定波长,如图3(右)所示。总之,我们已经证明了溶液合成的半导体纳米线可以用作传统场效应管结构中的通道,并且它们的高光吸收和高量子效率可以用于制造光电探测器。利用溶液合成的窄带隙半导体(PbS, PbSe)纳米线,光电探测器的光谱范围可以扩展到红外光谱范围,并可以在未来转移到柔性衬底上。[4]黄勇,段祥,崔勇,罗洪,等。Kim和C. Lieber,《自然》(伦敦)294,1313(2001)。[2]刘建军,刘建军,刘建军,等。启板牙。科学通报,30(2)(2000)。[3]周仁。Chang, V. Protansenko, M. Kuno, A. Singh和D. Jena,未发表(2006)。[4]张晓明,张晓明,张晓明,等。机械工程学报,2006,29(4)。图1:溶液合成的CdSe纳米线(左,中),以及溶液中接触垫之间的交流电场辅助介电泳排列(右)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信