Highly sensitive III–V nitride based piezoresistive microcantilever using embedded AlGaN/GaN HFET as ultrasonic detector

A. Talukdar, M. Qazi, G. Koley
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FET embedded microcantilevers are ideal for developing integrated electronic detection platform for biological and chemical analytes. GaN microcantilever with integrated AlGaN/GaN HFET deflection transducer offers very high mechanical, thermal, and chemical stability, in addition to extraordinary deflection sensitivity due to its strong piezoelectric properties. The piezoelectric property of III-V Nitrides causes a highly mobile (>;1500 cm2/Vs) two dimensional electron gas (2DEG) to form at the AlGaN/GaN interface, which gets strongly affected by the deflection induced strain. In addition, the electron mobility also changes due to the change in effective mass. The combined changes in 2DEG and mobility offer very high deflection sensitivity, verified through COMSOL finite element simulations and experimental observations. The effect of mechanical strain caused by microcantilever bending on the 2DEG and the AlGaN/GaN HFET characteristics has been reported experimentally [1] and theoretically [2] earlier, but this for the first time we have obtained such a high Gauge Factor. Microcantilevers were fabricated using III-V Nitride layers on Si(111). The layer structure consisted of i-GaN (2 nm)/ AlGaN (17.5 nm, 26% Al)/i-GaN (1 μm)/Transition layer (1.1 μm)/Si (111) substrate (500 μm). Fig. 1 (a) shows the SEM image of the fabricated device with the HFET shown in the inset. The HFET was fabricated with initial 200 nm mesa etching, followed by Ti(20 nm)/Al(100 nm)/Ti(45 nm)/Au(55 nm) metal stack deposition and rapid thermal annealing for ohmic contact formation. For gate contact, Ni(25 nm)/Au(375 nm) Schottky barrier was used. The fabricated microcantilever dimension is 350×50×2 μm. The GaN cantilever pattern was etched down using Ch based inductively coupled plasma etch process. Fig. 1 (b) shows the schematics of the experimental setup using our wire bonded device (shown as inset in Fig. 2) and Nanopositioner's (PI-611 Z). Fig. 2 shows the Id-V d characteristics of one of our best devices for different gate bias. In Fig. 3 the static bending performance is shown where the drain current is found to change by 6.3 % in magnitude, which gives a gauge factor of 3532. Both the downward and upward bending of cantilever exhibited similar changes. The movement of the nanopositioner was controlled using a Labview program, which was modified to also perform low frequency dynamic bending (up to 40 Hz). Fig. 4 shows the low frequency (0.5 Hz) response of a more typical device when the bending magnitude (both downward and upward) was 25 μm. We found that the low frequency upward and downward bending does not alter the gauge factor, and the response up to 40 Hz is also quite similar. We previously reported [3] a gauge factor of -38 (at Vg=0 V) and -860 in steady state and transient conditions, respectively. But our second generation devices consistently exhibit much higher gauge factor in both static and dynamic bending conditions at zero gate bias. We also extracted the AC response of the cantilevers using a miniature peizoactuator (PL055.31 from PI) and a lock-in amplifIer (SR 850). The ac response of the microcantilever, determined from direct contact oscillation of the piezo chip revealed a resonant peak of the cantilever at 45 KHz (Fig. 5) and a high quality factor of more than 200. The piezo chip was also used as an ultrasonic source and our microcantilever sensor was able to detect sub nm vibrational amplitude of the piezo chip from a distance of I cm. These results highlight the possibility of using III-V Nitride based piezoresistive microcantilevers as highly sensitive ultrasonic sensor for harsh environment, with wide ranging applications in acoustic spectroscopy and imaging.","PeriodicalId":6808,"journal":{"name":"70th Device Research Conference","volume":"1 1","pages":"19-20"},"PeriodicalIF":0.0000,"publicationDate":"2012-06-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"70th Device Research Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DRC.2012.6256983","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1

Abstract

Summary form only given.We report, for the first time, an ultra high gauge factor of more than 3500 observed using AlGaN/GaN Heterostructure Field Effect Transistor (HFET) embedded GaN piezoresistive microcantilever. In addition, the deflection transduction signal from the HFET was utilized to determine dynamic bending as well as AC frequency response of the cantilever. Finally, the piezoresistive microcantilver was used to detect very small acoustic pressure waves generated by a piezo chip oscillated at sub nm amplitude at the resonance frequency of the cantilever positioned 1 cm away, highlighting the utility of these cantilevers as highly sensitive ultrasonic transducers. FET embedded microcantilevers are ideal for developing integrated electronic detection platform for biological and chemical analytes. GaN microcantilever with integrated AlGaN/GaN HFET deflection transducer offers very high mechanical, thermal, and chemical stability, in addition to extraordinary deflection sensitivity due to its strong piezoelectric properties. The piezoelectric property of III-V Nitrides causes a highly mobile (>;1500 cm2/Vs) two dimensional electron gas (2DEG) to form at the AlGaN/GaN interface, which gets strongly affected by the deflection induced strain. In addition, the electron mobility also changes due to the change in effective mass. The combined changes in 2DEG and mobility offer very high deflection sensitivity, verified through COMSOL finite element simulations and experimental observations. The effect of mechanical strain caused by microcantilever bending on the 2DEG and the AlGaN/GaN HFET characteristics has been reported experimentally [1] and theoretically [2] earlier, but this for the first time we have obtained such a high Gauge Factor. Microcantilevers were fabricated using III-V Nitride layers on Si(111). The layer structure consisted of i-GaN (2 nm)/ AlGaN (17.5 nm, 26% Al)/i-GaN (1 μm)/Transition layer (1.1 μm)/Si (111) substrate (500 μm). Fig. 1 (a) shows the SEM image of the fabricated device with the HFET shown in the inset. The HFET was fabricated with initial 200 nm mesa etching, followed by Ti(20 nm)/Al(100 nm)/Ti(45 nm)/Au(55 nm) metal stack deposition and rapid thermal annealing for ohmic contact formation. For gate contact, Ni(25 nm)/Au(375 nm) Schottky barrier was used. The fabricated microcantilever dimension is 350×50×2 μm. The GaN cantilever pattern was etched down using Ch based inductively coupled plasma etch process. Fig. 1 (b) shows the schematics of the experimental setup using our wire bonded device (shown as inset in Fig. 2) and Nanopositioner's (PI-611 Z). Fig. 2 shows the Id-V d characteristics of one of our best devices for different gate bias. In Fig. 3 the static bending performance is shown where the drain current is found to change by 6.3 % in magnitude, which gives a gauge factor of 3532. Both the downward and upward bending of cantilever exhibited similar changes. The movement of the nanopositioner was controlled using a Labview program, which was modified to also perform low frequency dynamic bending (up to 40 Hz). Fig. 4 shows the low frequency (0.5 Hz) response of a more typical device when the bending magnitude (both downward and upward) was 25 μm. We found that the low frequency upward and downward bending does not alter the gauge factor, and the response up to 40 Hz is also quite similar. We previously reported [3] a gauge factor of -38 (at Vg=0 V) and -860 in steady state and transient conditions, respectively. But our second generation devices consistently exhibit much higher gauge factor in both static and dynamic bending conditions at zero gate bias. We also extracted the AC response of the cantilevers using a miniature peizoactuator (PL055.31 from PI) and a lock-in amplifIer (SR 850). The ac response of the microcantilever, determined from direct contact oscillation of the piezo chip revealed a resonant peak of the cantilever at 45 KHz (Fig. 5) and a high quality factor of more than 200. The piezo chip was also used as an ultrasonic source and our microcantilever sensor was able to detect sub nm vibrational amplitude of the piezo chip from a distance of I cm. These results highlight the possibility of using III-V Nitride based piezoresistive microcantilevers as highly sensitive ultrasonic sensor for harsh environment, with wide ranging applications in acoustic spectroscopy and imaging.
高灵敏度III-V型氮基压阻微悬臂梁,采用嵌入式AlGaN/GaN HFET作为超声波探测器
只提供摘要形式。我们首次报道了使用嵌入GaN压阻微悬臂的AlGaN/GaN异质结构场效应晶体管(HFET)观察到超过3500的超高测量因子。此外,利用HFET的挠度转导信号来确定悬臂梁的动态弯曲和交流频率响应。最后,使用压阻式微悬臂来检测由压电芯片在1厘米外悬臂的共振频率下以亚纳米振幅振荡产生的非常小的声压波,突出了这些悬臂作为高灵敏度超声波换能器的实用性。FET嵌入式微悬臂梁是开发生物和化学分析物集成电子检测平台的理想选择。集成了AlGaN/GaN HFET偏转传感器的GaN微悬臂具有非常高的机械、热和化学稳定性,此外,由于其强大的压电特性,GaN微悬臂还具有非凡的偏转灵敏度。III-V型氮化物的压电特性使其在AlGaN/GaN界面处形成高迁移率(> 1500 cm2/Vs)的二维电子气体(2DEG),受挠曲诱发应变的强烈影响。此外,电子迁移率也随着有效质量的变化而变化。通过COMSOL有限元模拟和实验观察,验证了2DEG和迁移率的综合变化提供了非常高的挠度灵敏度。微悬臂弯曲引起的机械应变对2DEG和AlGaN/GaN HFET特性的影响已经在实验[1]和理论[2]中有过报道,但这是我们第一次获得如此高的规范因子。在Si(111)表面采用III-V型氮化物层制备微悬臂梁。层结构由i-GaN (2 nm)/ AlGaN (17.5 nm, 26% Al)/i-GaN (1 μm)/过渡层(1.1 μm)/Si(111)衬底(500 μm)组成。图1 (a)显示了嵌入HFET的制造器件的SEM图像。首先采用200 nm的台面蚀刻工艺制备HFET,然后采用Ti(20 nm)/Al(100 nm)/Ti(45 nm)/Au(55 nm)金属堆沉积和快速热退火形成欧姆接触。栅极接触采用Ni(25 nm)/Au(375 nm)肖特基势垒。制备的微悬臂尺寸为350×50×2 μm。采用基于Ch的电感耦合等离子体刻蚀工艺刻蚀GaN悬臂图案。图1 (b)显示了使用我们的线键合器件(如图2所示)和Nanopositioner (pi - 611z)的实验装置的原理图。图2显示了我们最好的器件之一在不同栅极偏置下的Id-V - d特性。图3显示了静态弯曲性能,其中漏极电流的变化幅度为6.3%,测量系数为3532。悬臂梁的向下弯曲和向上弯曲都表现出相似的变化。使用Labview程序控制纳米逆变器的运动,该程序经过修改,也可以执行低频动态弯曲(高达40 Hz)。如图4所示,当弯曲幅度(上下)均为25 μm时,更为典型的器件的低频(0.5 Hz)响应。我们发现,低频上下弯曲不会改变测量因子,并且在40 Hz以下的响应也非常相似。我们之前报道过[3],在稳态和瞬态条件下,测量因子分别为-38 (Vg=0 V)和-860。但我们的第二代器件在零栅极偏置的静态和动态弯曲条件下始终表现出更高的测量因子。我们还使用一个微型peizoactuator(来自PI的PL055.31)和一个锁定放大器(SR 850)提取了悬臂梁的交流响应。由压电芯片的直接接触振荡确定的微悬臂梁的交流响应显示,悬臂梁在45 KHz处有一个谐振峰(图5),质量因数超过200。压电芯片也被用作超声波源,我们的微悬臂式传感器能够在1厘米的距离内检测到压电芯片的亚纳米振动幅度。这些结果强调了将III-V型氮化物压阻微悬臂用作恶劣环境下高灵敏度超声波传感器的可能性,在声学光谱和成像领域具有广泛的应用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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