利用二维电子气体的氢气传感器

Se Eun Kim, Hye Ju Kim, Sang Woon Lee
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引用次数: 0

摘要

氢(H2)由于其低点火能和高燃烧热,燃烧产物为H2O,被认为是一种清洁、环保的能源目前,氢气被认为是电动汽车运行最重要的能源。[2,3]但H2在浓度为4-75%时,不仅易燃而且易爆。不幸的是,由于氢气无色无味,人类无法检测到它。因此,为了人类的安全,需要开发灵敏的氢气传感器。[4,5] 2004年在氧化物异质结构界面上观察到二维电子气(2DEG)氧化异质结构中2DEG的模型体系为LaAlO3/SrTiO3异质结构的外延界面。最近,我们报道了在氧化物异质结构中使用非晶Al2O3顶层可以产生2DEG本文采用原子层沉积(ALD)技术在Al2O3/SrTiO3异质结构界面上制备了高性能H2气体传感器。钯(Pd)或铂(Pt)催化剂用于Al2O3/SrTiO3异质结构的顶部首先,我们将在Al2O3/SrTiO3异质结构界面上使用2DEG显示H2气敏性能。采用Al2O3/SrTiO3制备的H2气体传感器在室温下也具有较宽的H2浓度检测范围(5ppm-1%),且响应时间快。H2气体浓度越高,H2气体敏感性越高。Pd/Al2O3/SrTiO3传感器对Al2O3/SrTiO3的H2气体(3.2 eV)具有较快的响应时间,实现了透明气体传感器(可见光透过率>83%)。吸附H2气体改变了钯纳米粒子的2DEG电阻,这是因为H2的吸附调节了钯纳米粒子的功函数。功函数的改变引起了2DEG电阻的变化。详细的检测原理将在演示文稿中解释。采用2DEG异质结构(如AlGaN/GaN)的H2气体传感器是H2检测的另一个候选材料,因此,将AlGaN/GaN的H2气体传感器与Al2O3/SrTiO3传感器进行了比较。采用Al2O3/SrTiO3异质结构的氢气传感器对氢气的检测速度较慢,但灵敏度高(~30000%)。此外,还研究了在2DEG上Pt(或Pd)上使用原子层厚ZnO来增强AlGaN/GaN异质结构H2气体传感器的检测性能,从而提高了恢复时间。利用ALD生长出了原子层厚的ZnO层,这将在本报告中介绍。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Hydrogen Gas Sensors Using Two-Dimensional Electron Gas
Extended Abstract Hydrogen (H2) has been considered as a clean and environment-friendly energy source on account of its low ignition energy and high heat of combustion from which the combustion product is H2O.[1] Recently, H2 gas is regarded as the most important energy source for the operation of electrical vehicles.[2, 3] However, H2 is not only flammable but also explosive in the concentration of 4-75%. Unfortunately, it is impossible to detect H2 gas by human beings because of its colorless and odorless property. Therefore, a development of sensitive H2 gas sensor is required for human safety.[4,5] Two-dimensional electron gas (2DEG) was observed at the interface of oxide heterostructure in 2004.[6] The model system for 2DEG at the oxide heterostructure is epitaxial interface of LaAlO3/SrTiO3 heterostructure. Recently, we reported that 2DEG can be created at the oxide heterostructure by using amorphous Al2O3 top layer.[7] Here, we demonstrate highperformance H2 gas sensor using 2DEG at the interface of Al2O3/SrTiO3 heterostructure using atomic layer deposition (ALD). Palladium (Pd) or platinum (Pt) catalysts are used on top of the Al2O3/SrTiO3 heterostructure.[8] At first, we will show a H2 gas sensing performance using 2DEG at the interface of Al2O3/SrTiO3 heterostructure. The H2 gas sensor using Al2O3/SrTiO3 exhibited a wide sensing range of H2 concentration (5ppm-1%) even room temperature with fast response time. The more H2 gas concentration increased, the more H2 gas sensitive increased. The Pd/Al2O3/SrTiO3 sensor showed a fast response time to detect H2 gas (<30 s) at room temperature. Owing to a wide bandgap (>3.2 eV) of Al2O3/SrTiO3, a transparent gas sensor (transmittance >83% in the visible spectrum) was realized. 2DEG resistance is changed by adsorbing H2 gas because the work function of Pd nanoparticles is modulated by the H2 adsorption. Alteration of work function induced the change of the 2DEG resistance. The detailed detection principle will be explained in the presentation. H2 gas sensor using 2DEG at heterostructure such as AlGaN/GaN is another candidate for H2 detection, thus, H2 sensor using AlGaN/GaN is compared with Al2O3/SrTiO3 sensor. H2 gas sensor using AlGaN/GaN heterostructure showed a slow H2 detection speed, but superior sensitivity (~30000%) compared to the Al2O3/SrTiO3 sensor. In addition, enhanced detection performances of H2 gas sensor with AlGaN/GaN heterostructures using atomic-layer-thick ZnO on Pt (or Pd) on 2DEG are addressed, which improved a decrease of recovery time. The atomic-layer-thick ZnO layer was grown by ALD which will be introduced in the presentation.
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