氧化钒薄膜材料及非制冷红外探测器微结构设计的研究
详细信息    本馆镜像全文|  推荐本文 |  |   获取CNKI官网全文
摘要
红外探测器发展的方向是非制冷、低成本以及小型化。基于热敏电阻的测辐射热计式红外探测器是主流的低成本非制冷红外热探测器之一,近年来越来越受到各国研究者的关注。对其的研究集中在两个方面:一是不断提高探测材料性能;再一个是探测器热绝缘结构方面的研究和改进以获得高响应的探测器。
     具有优异热敏性能的氧化钒薄膜材料是非制冷测辐射热计红外探测器的首选的热敏电阻材料。制备合适的薄膜电阻值且具有大的电阻温度系数(TCR)的氧化钒薄膜是实现高探测率红外测辐射热计的基础。本文利用新颖的对靶反应磁控溅射工艺制备了氧化钒薄膜材料,运用正交实验进行了工艺参数的研究,通过选择不同的工艺参数和不同的参数水平,得到了氩氧比例、溅射功率、工作气压、基片温度、基片类型以及真空退火等条件对氧化钒薄膜性能的影响,确定了最佳工艺参数。对得到的氧化钒薄膜的组成、结构和性能进行了测试分析。扫描电子显微镜(SEM)原子力显微镜(AFM)形貌分析表明薄膜具有均匀致密的表面,X射线光电子能谱分析(XPS)确定了其成分组成主要为V_2O_5、VO_2和少量的V_2O_3;对氧化钒薄膜电阻温度特性的研究表明,薄膜成分中各价态钒离子的比例对TCR和室温电阻有着重要的影响。钒的总体价态越高,室温电阻越大,TCR也越大;TCR较高并且阻值适当的样品中,钒的总体价态接近+4价。在常用作微测辐射热计MEMS结构层材料的氮化硅基底上沉积氧化钒薄膜所确定的最佳工艺条件为工作气压:2.0 Pa,氩氧流速比:Ar:O2 =48:0.5,基片温度:200℃,溅射功率: 210W。该工艺条件下薄膜材料在室温附近具有合适的薄膜电阻(14KΩ/□左右)以及高的温度电阻系数(-3.17%/℃),所研制得到的氧化钒薄膜工艺重复性好,可以和半导体工艺兼容,非常适合于非致冷红外测辐射热计探测器应用。
     多孔硅材料作为牺牲层材料或绝热层材料均可为探测器单元的绝热结构制作提供新思路和解决途径。对具有多孔硅热绝缘层的氧化硅基底以及直接在硅衬底的氧化硅基底上淀积的氧化钒薄膜热敏特性进行对比研究表明,采用多孔硅结构可达到很好的绝热效果。另外,研究表明采用双槽电化学法制备的多孔硅腐蚀速率高,腐蚀后获得具有与掩模相同的表面轮廓和平整的底面的凹槽,适于用作牺牲层材料。
     利用有限元方法指出微测辐射热计微桥结构的设计思路,热分布分析表明对角支撑的探测器单元具有最好的温度梯度均匀性。对微桥的一些关键尺寸参数在规定的取值空间内进行建模优化设计,并分析了这些参数对位移形变和应力的影响。
The trends of infrared(IR) detector are being uncooled, cheaper and more convenient. Bolometer which is a dominant low-cost uncooled thermal infrared detector based on thermistor have attached more and more attention by researchers around the world. Emphases are focused on two aspects, one is to improve the property of thermistor material continually to obtain high detector performace; the other is the research and improvement on thermal isolation structure of detector.
     Vanadium oxide with outstanding thermal sensing property is an ideal thermistor material for bolometer application and the fabrication of vanadium oxide thin film with high temperature coefficient of resistance (TCR) and suitable film resistance is the base of high detectivity of microbolometer. In this paper, Vanadium oxide thin film with nanostructure was deposited by novel facing targets DC reactive sputtering technique using V metal as target and the effect of deposition parameters including ratio of Ar/O2, sputtering power, work pressure, substrate temperature, sustrate types and vacuum annealing on the performance of vanadium oxide thin films is analyzed by choosing different level of these parameters in the orthogonal experiment. Optimal deposition parameters were defined. X-ray photoelectron spectroscopy analysis revealed the vanadium oxygen state of the film, which included V2O5、VO2 and a few V2O3. Atomic force microscopy surface morphology indicated a planar and compact film surface. TCR becomes higher (lower) as the higher (lower) sheet resistance. In the VOx films with high TCR and moderate sheet resistance, the average valence of vanadium is about +4. The optimal deposition parameters of vanadium oxide film on Si3N4 substrate, which is a common MEMS structure material in microbolometer use, were defined as follow: Working pressure: 2.0 Pa, gas flow ratio: Ar:O2 =48:0.5, substrate temperature 200℃, sputtering power: 210W. The temperature coefficient of resistance (TCR) as-deposited was high up to -3.17%/℃and the sheet resistance was about 14KΩ/□around room temperature. This deposition process has nice repetitivity and can be compatible with semiconductor process, which implied promising application in uncooled microbolometer infrared (IR) detectors.
     porous silicon,used as sacrificial layers or thermal insulator in the multi-layer structure can provide new methods to the fabrication of thermal isolation structure, the contrast result of the thermal sensing property of VOx resistance under a small power input deposited on porous silicon substrate and silicon substrate revealed good thermal isolation property of porous silicon layer. Otherwish, Porous silicon prepared by double-cell electrochemical etching has a high removing speed and it is found a trench was formed with almost the same pattern with the mask and flat bottom after etching, which implicit it is suitable for sacrificial material application.
     The finite element method was used in the design of microbridge structure for mcirobolometer, the temperature distributing analysis indicate the best uniformity in the structure supporting on diagonally position. Optimizing analysis of the Key scale parameters of microbridge was carried out in the seting scale space using a finite element model, the effect of these parameters on deformation was analysed.
引文
[1]孙志君,刘俊刚,欧代永,红外焦平面陈列技术的新军事装备的应用,传感器世界,2004,10(11):6~12
    [2]Antoni Rogalski, Review Infrared detectors: status and trends, Progress in Quantum Electronics, 2003, 27: 59~210.
    [3]袁继俊,红外探测器的研究,生产和应用,激光与红外,1998,28(5):288~291
    [4]Antoni Rogalsk,Toward third generation HgCdTe infrared detectors,Journal of Alloys and Compounds, 2004, 371: 53~57
    [5]朱惜辰,红外探测器的进展,红外技术,1999,21(6):12~15
    [6]陈继述,胡燮荣,徐平茂,红外探测器,北京:国防工业出版社,1986:1~3
    [7]孙志君,红外焦平面阵列技术的未来二十年传感器世界,2002,8(11):1~8
    [8]刘贤德,红外系统设计基础,武汉:华中工学院出版社,1985:1~10
    [9]常本康,蔡毅,红外成像阵列与系统,北京:科学出版社,2006,18~20
    [10] L.R.Senesac, J.L.Corbeil, S.Rajic et al, IR imaging using uncooled microcantilever detectors, Ultramicroscopy, 2003, 97: 451–458.
    [11]吴诚,苏君红,潘顺臣 等,非致冷红外焦平面技术评述(上),红外技术,1999,21(1):6~9
    [12]吴诚,苏君红,潘顺臣 等,非致冷红外焦平面技术评述(下),红外技术,1999,21(2):1~3
    [13]陈伯良, 孙维国, InSb凝视红外焦平面组件研制和应用, 红外与激光工程2002, 31(5): 419~423
    [14]何力,陈路,吴俊 等, 应对第三代红外焦平面技术挑战的HgCdTe分子束外延,半导体学报,2006,27(3):381~387
    [15]朱西安,孙浩,王成刚 等,HgCdTe微台面红外焦平面技术研究,激光与红外,2005,35(11):826~828
    [16]程开富,国内外MSSBIRFPA的发展现状及其应用,集成电路通讯,2003,21(4):8~12
    [17]M.N. Gurnee, M. Kohin, R. Blackwell, et al. Developments in uncooled IR technology at BAE Systems, Proceedings of SPIE, 2001, 4369:287~296.
    [18]J.L. Tissot, IR detection with uncooled sensors, Infrared Physics & Technology, 2004, 46: 147~153
    [19]刘卫国,金娜,集成非制冷热成像探测阵列,北京,国防工业出版社,2004: 39~40.
    [20]刘世建,徐重阳,曾祥斌,非制冷红外焦平面阵列用探测材料,电子元件与材料,2002,21(10):22~24
    [21]A. Jahanzeb, C.M. Travers, Z. Celik-Butler, et al. A semiconductor YBaCuO microbolometer for room temperature IR imaging, IEEE Transactions on Electron Devices, 1997, 44:1795~1801.
    [22]吕宇强,胡明,吴淼,等, 热红外探测器的最新进展,压电与声光,2006, 28(4):407~410
    [23]Naoki ODA, Yutaka TANAKA, Tokuhito SASAKI, et al. Preformance of 320×240 Bolometer -Type Uncooled Infrared Detector, NEC Res. & Develop, 2003, 44(2):170~174.
    [24]S.B. Wang, S.B. Zhou, X.J. Yi. Preparation of homogeneous VOX thin films by ion beam sputtering and annealing process, Vacuum, 2004, 75:85~90.
    [25]Mei Pan, Hongmei Zhong, Shaowei Wang. Properties of VO2 thin film prepared with precursor VO(acac)2, Journal of Crystal Growth,2004, 265:121~126
    [26]吴淼,胡明,温宇峰. 基片温度对氧化钒薄膜结构与电性能的影响[J].压电与声光,2004,26(6):471~473.
    [27]吕宇强,胡明 等,红外微测辐射热计用纳米氧化钒薄膜的制备和性能研究,《纳米技术与精密工程》2006, 4(3):221~224
    [28]刘卫国 金娜 集成非制冷热成像探测阵列 北京 国防工业出版社 2004 236~238.
    [29]Hongchen Wang, Xinjian Yi, Guang Huang. IR microbolometer with self-supporting structure operating at room temperature[J].Infrared Physics & Technology,2004,45: 53~57.
    [30]王亚珍,朱文坚,微机电系统(MEMS)技术及发展趋势,机械设计与研究,2004,20(1):10~12
    [31]Stephen D. Senturia,微系统设计(刘泽文等译),北京:电子工业出版社,2004:2~4.
    [32]李德胜,关佳亮,石照耀 等,微纳米技术及其应用,北京:科学出版社,2005,2~13.
    [33]李兰,刘铮,邹德恕,等,MEMS 技术用于红外器件制作,激光与红外,2003,33(3),212~214
    [34]Jongeun Choi, Joji Yamaguchi, Simon Morales,et al, Design and control of a thermal stabilizing system for a MEMS optomechanical uncooled infrared imaging camera, Sensors and Actuators A, 2003,104:132~142.
    [35]M. Navarro, J.M. López-Villegas, J. Samitier, et al., Improvement of the porous silicon sacrificial-layer etching for micromachining applications, Sensors andActuators, 1997, A62(1/3): 676~679
    [36] Monticone E., Boarino L., Lérondel G., et al. Properties of metal bolometers fabricated on porous silicon. Applied Surface Science, 1999, 142(1-4): 267~271
    [37]W. Lang, P. Steiner and H. Sandmaier, Porous silicon: a novel material for Microsystems, Sensors and Actuators, 1995, 51(1): 31~36
    [38]P. Steiner, W. Lang, Micromachining applications of porous silicon, Thin Solid Films, 1995, 255(1-2): 52~58
    [39]Partlow, DP, Gurkovich, SR, Radford, KC, et al.,Switchable vanadium oxide films by a sol-gel process, Journal of Applied Physics, 1991, 70(1): 443~452
    [40]Verkelis J.,Bliznikas Z.,Breiv? K.,,et al.,Vanadium oxides thin films and fixed-temperature heat sensor with memory,Sensors and Actuators A,1998,68(1-3): 338~343
    [41]汤兆胜、孙玉琴、范正修,V2O5薄膜用作SO2气敏传感器,功能材料,2002,33(1):52~59
    [42] Jiguang Zhang, Ping Liu,Vanadium oxide thin-film cathodes for lithium rechargeable battery applications,Journal of Dalian University of Technology,1998,38(1):19~25
    [43]Y.S.Yoon,J.S.Kim,S.H.Choi,Structural and electrochemical properties of vanadium oxide thin films grown by d.c. and r.f. reactive sputtering at room temperature,Thin Solid Films, 2004, 460: 41~47
    [44]G. Golan,A. Axelevitch,B. Sigalov,et al.,Metal–insulator phase transition in vanadium oxides films,Microelectronics Journal, 2003, 34: 255~258
    [45]Chen, Sihai,Ma, Hong,Yi, Xinjian,et al.,Optical switch based on vanadium dioxide thin films,Infrared Physics and Technology, 2004, 45(4): 239~242
    [46]Wang, S.B.,Xiong, B.F.,Zhou, S.B.,et al.,Preparation of 128 element of IR detector array based on vanadium oxide thin films obtained by ion beam sputtering,Sensors and Actuators A: Physical, 2005, 117(1):110~114
    [47]袁宁一,李金华,林成鲁,氧化钒薄膜的制备方法及结构性能,江苏石油化工学院学报,2000,12(4):1~4
    [48] S. Surnev, M.G. Ramsey, F.P. Netzer, Vanadium oxide surface studies, Progress in surface science, 73(2003): 117~16.
    [49]潘梦霄,曹兴忠,李养贤 等,氧化钒薄膜微观结构的研究,物理学报,2004,53(6):1956~1960
    [50]周静,闵新民,V2O5复合薄膜材料的电子结构研究,硅酸盐学报,2002,30(2):208~211
    [51]F. J. Morin, Oxides Which Show a Metal-to-Insulator Transition at the Neel Temperature, Phys. Rev. Lett, 1959,3:34~36
    [52]许旻,邱家稳,何延春 等,二氧化钒薄膜的结构、制备与应用,真空与低温,2001,7(3):136~138
    [53]徐毓龙,氧化物与化合物半导体基础,西安:西安电子科技大学出版社,1991,268~275
    [54]刘金城、鲁建业、田雪松 等,二氧化钒薄膜研究的最新进展,哈尔滨工业大学学报,2002,34(4):570~572
    [55]徐时清、赵康、谷臣清 等,掺杂VO2相变薄膜的突变特性研究,硅酸盐学报,2002,30(5):637~640
    [56]Y.S.Yoon,J.S.Kim,S.H.Choi,Structural and electrochemical properties of vanadium oxide thin films grown by d.c. and r.f. reactive sputtering at room temperature,Thin Solid Films 460 (2004):41~47
    [57]吴淼,胡明,张之圣等,直流对靶溅射制备氧化钒薄膜的研究,天津市真空学会2004年度学术年会,2004,12
    [58]周少波,王双保,陈四海 等,反应离子束溅射沉积和还原退火工艺制备VOx多晶薄膜,材料开发与应用,2004,19(6):20~21
    [59]李志栓,李静,吴孙桃 等,射频磁控溅射方法制备氧化钒薄膜的研究,厦门大学学报,2005,44(1):37~40
    [60]吴淼,胡明,张之圣 等,真空蒸发法制备氧化钒薄膜的研究,硅酸盐通报,2005,24(1):17~19
    [61]Hubl,GK,唐源,离子束辅助沉积的基本原理: Ⅱ. 离子和蒸发物通量的绝对校准,国外核聚变与等离子体应用,1991(5):79~90
    [62]R T Rajendra Kumar, B Karunagaran, D Mangalaraj, et al, Room temperature deposited vanadium oxide thin films for uncooled infrared detectors,Materials Research Bulletin, 2003, 38: 1235~1240
    [63]R T Rajendra Kumar, B Karunagaran, D Mangalaraj, et al, Study of a pulsed laser deposited vanadium oxide based microbolometer array, Smart Materials and Structures, 2003, 12:188~192
    [64]K.R.Speck, Vanadium dioxide films grown from vanadium tetraisopropoxide by the sol-gel process, Thin Solid Films, 1988, 1651: 317~322
    [65]许旻,贺德衍,脉冲溅射V2O5薄膜结构和性能研究,光学学报,2004,24(6):743~746
    [66]Chenmou Zheng, Xinmin Zhang, Jianhui Zhang,Preparation and Characterization of VO2 Nanopowders,Journal of Solid State Chemistry, 2001, 156: 274~280
    [67]刘粤惠,刘平安,X射线衍射分析原理与应用,北京:化学工业出版社,2003,1~5
    [68]袁宁一、李金华、林成鲁,氧化钒薄膜的结构、性能及制备技术的相关性,功能材料,2001,32(6):572~575
    [69]李金华,袁宁一,林成鲁 等,用离子束增强沉积从V2O5粉末制备高热电阻温度系数VO2薄膜,物理学报,2002,51(8):1788~1792
    [70]杨邦朝,王文生,薄膜物理与技术,成都:电子科技大学出版社,1994,82~83
    [71]杨邦朝,王文生,薄膜物理与技术,成都:电子科技大学出版社,1994,60~61
    [72]吴淼,胡明,吕宇强 等,常温反应磁控对靶溅射制备高 TCR 氧化钒薄膜的研究,天津大学学报,2006,39(7):806~809
    [73]周围,林理彬,真空退火引起的 VOx 薄膜生长过程的变价问题研究,功能材料,1997,28(6):609~611
    [74]卢勇,林理彬,真空还原制备的VO2热致相变薄膜光学性质研究,激光杂志,2001,22(3):8~10
    [75]周围,林理彬,真空退火引起的VOx薄膜生长过程的变价问题研究,功能材料,1997,28(6):609~611
    [76]Michael Quirk,Julian Serda,半导体制造技术(韩郑生等译),北京:电子工业出版社,2004,125~132
    [77]刘振学,黄仁和,田爱民,实验设计与数据处理,北京:化学工业出版社,2005,62~74
    [78]许旻,邱家稳,赵印中 等,VO2薄膜制备工艺及电阻开关特性研究,中国空间科学技术,2001,12(6):64
    [79]刘吉平, 郝向阳,纳米科学与技术,北京:科学出版社,2002.
    [80]R T Rajendra Kumar, B Karunagaran, D Mangalaraj, et al. Properties of pulsed laser deposited vanadium oxide thin film thermistor, Materials Science in Semiconductor Processing, 2003, 6: 375~377.
    [81]田彬,胡明,马家志 等,多孔硅制备方法新进展及在微传感器中的应用,压电与声光,2003,25(6):521~524
    [82]Roussel Ph, Lysenko V, Remaki B, et al, Thick oxidised porous silicon layers for the design of a biomedical thermal conductivity microsensor, Sensors and Actuators, 1999, A74(1-3): 100~103.
    [83]Tabata O, Fast-response silicon flow sensor with an on-chip fluid temperature sensing element, IEEE Transactions on Electron Devices, 1986, ED-33(3): 361~365.
    [84]H.SAHA, C.PRAMANIK, Porous Silicon-Based Sensors: Prospects and Challenges, Material and manufacturing Processes,2006, 21: 239~246.
    [85]王清涛,李清山,多孔硅及其应用研究展望,辽宁大学学报:自然科学版,2001,28(4):301~304
    [86]G. Di Francia, A.Citarella, Kinetic of the growth of chemically etched porous silicon, Journal of Applied Physics, 1995, 77 (7): 3549~3551
    [87] Michael T. Kelly, Jonathan K.M. Chun and Andrew B. Bocarsly, High efficiency chemical etchant for the formation of luminescent porous silicon, Applied PhysicsLetters, 1994, 64(13): 1693~1695
    [88]G. Lammel, Ph. Renaud, Free-standing, mobile 3D porous silicon microstructrues, Sensors and Actuators, 2000, A85 (1/3): 356~360
    [89]刘卫国,金娜,集成非制冷热成像探测阵列,北京:国防工业出版社,2004: 246~250.
    [90] Saeed Moaveni,有限元分析-ANSYS理论与应用(第二版) (王崧译),北京:电子工业出版社,2005,1~6
    [91]宋勇,艾宴清,梁波精,精通ANSYS 7.0有限元分析,北京:清华大学出版社,1~8
    [92]李黎明,ANSYS有限元分析实用教程,北京:清华大学出版社,2006:10~23
    [93]沈晓燕,顾文韵,皮德富,微测辐射热计响应率的数值分析,红外与激光工程,2003,32(1):105~108
    [94]陈建国,郭群英,邢昆山,测辐射热计的微桥研制和VOx膜成膜研究,半导体技术,2002,27(1):70~73
    [95]杜晓晴,常本康,微测辐射热计的热隔离结构设计,激光与红外,2002, 24(3):265~267
    [96]顾文韵,皮德富,周士源,测辐射热计探测器中温度场有限元计算分析,兵工学报,2002,23 (1):109~111
    [97]王享田,宋建伟,吴志明 等,微测辐射热计FPA的热学分析,半导体光电增刊:2005,26,37~40
    [98] 小飒工作室,最新经典ANSYS及Workbench教程,北京:电子工业出版社 2004:644~663
    [99]郭仁生,苏君,卢洪胜,优化设计应用,北京:电子工业出版社,2003:1~2
    [100]李黎明,ANSYS有限元分析实用教程,北京:清华大学出版社,2006:338~339
    [101]陈宝林,最优化理论与算法,北京:清华大学出版社,2005,203~322

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700