利用微型Lamb波传感器研究薄膜—流体的相互作用
详细信息    本馆镜像全文|  推荐本文 |  |   获取CNKI官网全文
摘要
微型Lamb波传感器具有高灵敏度、低损耗、多模式特性,是研究薄膜-流体的界面相互作用最有力的工具之一,尤其在交叉学科且尚未探讨的领域,如气体传感、空气动力学、多参数解耦等领域。本论文从理论上和实验上,系统地探讨了微型Lamb波传感器在薄膜-流体(气体和液体)界面相互作用中的应用。主要研究内容如下:
     ?采用势能函数结合边界耦合模型,分析Lamb波传播过程中的薄膜-流体界面相互作用,重点计算了色散特性曲线、分子位移、应力、坡印廷矢量、群速度、能量速度等。针对微型Lamb波传感器的薄膜纵向长度的有限性,建立相应的简化模型,直观、准确地揭示了微型Lamb波的模式分布,突破和拓宽了以往对微型Lamb波传感器的模式分布的认识,为研究薄膜-流体的界面相互作用奠定了基础。
     ?从理论上和实验上研究了薄膜-气体界面处的消逝波和漏波对气体的响应。结果显示:当气体变化时,低频下的A0模式(消逝波)仅表现为相对频率的移动,且变化曲线呈现“U”型;高频下的A0模式(漏波)表现为的Q值(品质因数)的变化,即Q值随着Lamb波的相位速度接近气体的声速而快速降低。S_0模式对气体的变化不敏感,故S_0模式是作为参考模式的理想选择
     ?利用薄膜-气体界面处的声场(消逝波和漏波)与气体的流动边界层的相互作用,给出流动气体的相关参数。对于消逝波,气流的边界层厚度和消逝波的穿透深度决定着灵敏度的大小。当Lamb的相位速度接近于气体的声速时,气流的速度和方向明显影响消逝波的声场分布。对于漏波,气流对Lamb波的传播几乎没有任何影响。
     ?利用Lamb波的多个模式在薄膜-液体界面处的特性不同,对液体的多个物理参数进行解耦(密度、声速、粘度等),从而定量地给出液体的成分和组分。结合A01模式(低频A0模式的基模)和A03模式(A0模式的3次谐振模式)可分别解耦出液体的密度和声速。密度确定后,通过测量S_0模式的幅值响应,解耦出液体的粘度。
Micro Lamb wave sensor is one of useful tools to study the membrane-fluid interaction, especially in interdisciplinary and not yet explored areas, such as gas sensing, aerodynamics, the multi-parameters decoupling and so on. This is because micro Lamb wave sensor holds high sensitivity, low losses and multi-modes. This thesis deals with the membrane-fluid interaction with micro Lamb wave sensor theoretically and experimentally. The details are described as follows:
     In theory, combinations of the potential function method and the boundary conditions at all interfaces are used to analyze the membrane-fluid interaction. There are several aspects of this problem can addressed, including the displacement, the stress, velocity dispersion curve, Poynting vector, group velocity, energy velocity and so on. In the case of micro Lamb wave sensor, the resonant modes can be excited and worked simultaneously with the traveling modes, as the membrane is width limited and not large enough comparing with the wavelength of Lamb waves. The established model can reveal the mode distributions in micro Lamb wave device clearly and accurately. These works provide insight into the understandings of the modes in micro Lamb wave device, which is useful for further experiments.
     The gases effects on the evanescent wave and leaky wave near the membrane-gas interface are studied. The relative frequency shifts in the low frequency range of the A0 mode (evanescent wave, EW) is rather important and the shape of the curve looks like‘U’shape. In the high frequency range of this mode (leaky Lamb wave, LLW), the quality factor decreases rapidly when the Lamb wave phase velocity approaches the gas sound velocity. The S0 mode shows immune to gas loading, which can be used as reference mode. This provides theoretical and experimental works for related fields in gas sensing.
     The application of membrane-gas interaction in aerodynamics is investigated theoretically and experimentally. The interaction between the gas flow boundary layer and the acoustic sound field (EW and LLW) at the membrane-gas interface can give out the parameter in the gas flow. In the EW case, the thickness of the gas flow boundary layer and the penetration depth of the evanescent wave are the two factors determining the sensitivity. When the Lamb wave phase velocity approaches the gas sound velocity, the gas flow effect is clearly observed. In the LLW case, it is shown experimentally that the gas flow has not evident effects on Lamb wave’s propagations.
     At the membrane-liquid interface, the effects of different physical parameters (density, sound velocity, viscosity, etc) on the modes’propagations are studied. The liquid ingredients and components can be indentified quantitatively. Combination of the relative frequency shifts of the A01 mode (low frequency of A0 mode) and the A03 mode (the third harmonic wave of the A01 mode), the density and the sound velocity of the liquid can be decoupled. With the determined density, the amplitude in the S0 mode can decouple the viscosity of the liquid.
引文
[1] D. Ballantine, et al., Acoustic wave sensors: theory, design, and physico-chemical applications: Academic Press San Diego, 1996.
    [2] M. Hoummady, et al., "Acoustic wave sensors: design, sensing mechanisms and applications," Smart Materials & Structures, vol. 6, pp. 647-657, Dec 1997.
    [3] Y. Q. Fu, et al., "Recent developments on ZnO films for acoustic wave based bio-sensing and microfluidic applications: a review," Sensors and Actuators B: Chemical, vol. 143, pp. 606-619, 2010.
    [4] D. W. Galipeau, et al., "Surface acoustic wave microsensors and applications," Smart Materials & Structures, vol. 6, pp. 658-667, Dec 1997.
    [5] L. Ralf and H. Peter, "Transduction mechanism of acoustic-wave based chemical and biochemical sensors," Measurement Science and Technology, vol. 14, p. 1854, 2003.
    [6] J. W. Grate, et al., "Acoustic wave microsensors," Analytical Chemistry, vol. 65, pp. 940A-948A, 1993.
    [7] N. Setter, et al., "Ferroelectric thin films: Review of materials, properties, and applications," Journal of Applied Physics, vol. 100, p. 46, Sep 2006.
    [8] P. Muralt, "Ferroelectric thin films for micro-sensors and actuators: a review," Journal of Micromechanics and Microengineering, vol. 10, p. 136, 2000.
    [9] S. Trolier-McKinstry and P. Muralt, "Thin Film Piezoelectrics for MEMS," Journal of Electroceramics, vol. 12, pp. 7-17, 2004.
    [10] S. Tadigadapa and K. Mateti, "Piezoelectric MEMS sensors: state-of-the-art and perspectives," Measurement Science and Technology, vol. 20, 2009.
    [11] L. Rayleigh, "On Waves Propagated along the Plane Surface of an Elastic Solid," Proc. London Math. Soc., vol. s1-17, pp. 4-11, November 1, 1885 1885.
    [12] R. M. White and F. W. Voltmer, "Direct piezoelectric coupling to surface elastic waves," Applied Physics Letters, vol. 7, pp. 314-316, 1965.
    [13] T. M. A. Gronewold, "Surface acoustic wave sensors in the bioanalytical field: Recent trends and challenges," Analytica Chimica Acta, vol. 603, pp. 119-128, 2007.
    [14] A. Arnau, Piezoelectric transducers and applications: Springer Verlag, 2008.
    [15] B. A. Cavic, et al., "Acoustic waves and the study of biochemical macromolecules and cells at the sensor-liquid interface," Analyst, vol. 124, pp. 1405-20, Oct 1999.
    [16] A. Janshoff, et al., "Piezoelectric Mass-Sensing Devices as Biosensors - An Alternative to Optical Biosensors?," Angewandte Chemie, vol. 39, pp. 4004-4032, 2000.
    [17] G. N. M. Ferreira, et al., "Acoustic wave biosensors: physical models and biological applications of quartz crystal microbalance," Trends in Biotechnology, vol. 27, pp. 689-697, 2009.
    [18] T. Nomura and M. Okuhara, "Frequency shifts of piezoelectric quartz crystals immersed in organic liquids," Analytica Chimica Acta, vol. 142, pp. 281-284, 1982.
    [19] B. Eggins, Chemical sensors and biosensors: Wiley, 2002.
    [20] G. Wingqvist, "Thin film electroacoustic devices for biosensor applications," Ph.D, Department of Engineering Sciences, Solid State Electronics, Uppsala University, Uppsala,Sweden, 2009.
    [21] S. J. Martin, et al., "Characterization of a quartz crystal microbalance with simultaneous mass and liquid loading," Analytical Chemistry, vol. 63, pp. 2272-2281, 1991.
    [22] T. Grudkowski, et al., "Fundamental mode VHF/UHF minature acoustic resonators and filters on silicon," Applied Physics Letters, vol. 37, p. 993, 1980.
    [23] K. Lakin and J. Wang, "Acoustic bulk wave composite resonators," Applied Physics Letters, vol. 38, p. 125, 1981.
    [24] Y.-R. Kang, et al., "Air-gap type film bulk acoustic resonator using flexible thin substrate," Sensors and Actuators A: Physical, vol. 117, pp. 62-70, 2005.
    [25] J. Enlund, et al., "Solidly mounted thin film electro-acoustic resonator utilizing a conductive Bragg reflector," Sensors and Actuators A: Physical, vol. 141, pp. 598-602, 2008.
    [26] H. Zhang and E. Kim, "Micromachined acoustic resonant mass sensor," Journal of Microelectromechanical Systems, vol. 14, pp. 699-706, 2005.
    [27] J. Weber, et al., "Shear mode FBARs as highly sensitive liquid biosensors," Sensors and Actuators A: Physical, vol. 128, pp. 84-88, 2006.
    [28] B. Jakoby and M. J. Vellekoop, "Properties of Love waves: applications in sensors," Smart Materials & Structures, vol. 6, pp. 668-679, Dec 1997.
    [29] A. Love, Some problems of geodynamics: Cornell University Library, 1911.
    [30] D. H. Dinh, et al., "Novel optimized biofunctional surfaces for Love mode surface acoustic wave based immunosensors," Sensors and Actuators B: Chemical, vol. 146, pp. 289-296, 2010.
    [31] B. Auld, Acoustic fields and waves in solids: RE Krieger, 1990.
    [32] J. Du, et al., "A study of Love-wave acoustic sensors," Sensors and Actuators A: Physical, vol. 56, pp. 211-219, 1996.
    [33] M. Badi, "Capacitive micromachined ultrasonic lamb wave transducers," stanford university, 2004.
    [34] L. Pochhammer, "Biegung des kreiscylinders-fortpflanzungs-geschwindigkeit kleiner schwingungen in einem kreiscylinder," Journal für die reine und angewandte Mathematik, vol. 81, pp. 324-336, 1876.
    [35] H. Lamb, "On Waves in an Elastic Plate," Proceedings of the Royal Society of London, Series A: Mathematical and Physical Sciences, vol. 93, pp. 114-128, 1917.
    [36] S. P. Timoshenko, "LXVI. On the correction for shear of the differential equation for transverse vibrations of prismatic bars," Philosophical Magazine Series 6, vol. 41, pp. 744 - 746, 1921.
    [37] S. P. Timoshenko, "X. On the transverse vibrations of bars of uniform cross-section," Philosophical Magazine Series 6, vol. 43, pp. 125 - 131, 1922.
    [38] H. Reissner, "Der senkrechte und schr?ge Durchtritt einer in einem flüssigen Medium erzeugten ebenen Dilatations-Welle durch eine in diesem Medium befindliche planparallele feste Platte," Helvetica Physica Acta, vol. 11, pp. 140-155, 1938.
    [39] G. J., "über den Schalldurchgang durch Metallplatten in Flüssigkeiten bei schr?gem Einfall einer ebenen Welle," Akustische Zeitschrift, vol. 8, pp. 145-168, 1943.
    [40] F. Sanders, "Transmission of sound through thin plates," Canadian Journal of Research, vol. 17, pp. 179-193, 1939.
    [41] R. D. Fay and O. V. Fortier, "Transmission of Sound through Steel Plates Immersed in Water," The Journal of the Acoustical Society of America, vol. 23, pp. 339-346, 1951.
    [42] M. F. M. Osborne and S. D. Hart, "Transmission, Reflection, and Guiding of an Exponential Pulse by a Steel Plate in Water. I. Theory," The Journal of the Acoustical Society of America, vol. 17, pp. 1-18, 1945.
    [43] I. Viktorov, "Ultrasonic lamb waves," Sov. Phys. Acoust, vol. 11, pp. 1-14, 1965.
    [44] K. Toda, "Frequency characteristics of an interdigital transducer for Lamb wave excitation," Journal of Applied Physics, vol. 45, pp. 5136-5140, 1974.
    [45] S. W. Wenzel, "Applications of ultrasonic Lamb waves," Ph.D., Department of Electrical Engineering and Computer Sciences, University of California, Berkeley, 1992.
    [46] T. Laurent, et al., "Lamb wave and plate mode in ZnO/silicon and AlN/silicon membrane: Application to sensors able to operate in contact with liquid," Sensors and Actuators A: Physical, vol. 87, pp. 26-37, 2000.
    [47] Y. Wu, et al., "Investigations on excitation and detection methods for Lamb wave sensors," Sensors and Actuators A: Physical, vol. 100, pp. 214-222, 2002.
    [48] H. Jia, et al., "Improvement of Lamb waves sensors: Temperature sensitivity compensation," Sensors and Actuators A: Physical, vol. 121, pp. 321-326, 2005.
    [49] F. Li, et al., "Temperature compensation of lamb wave sensor by combined antisymmetric mode and symmetric mode," Applied Physics Letters, vol. 92, p. 074101, 2008.
    [50] F. Li, et al., "Measurements of evanescent wave in a sandwich Lamb wave sensor," Applied Physics Letters, vol. 93, pp. 174101-3, 2008.
    [51] P. K. Sekhar, et al., "A low loss flexural plate wave (FPW) device through enhanced properties of sol-gel PZT (52/48) thin film and stable TiN-Pt bottom electrode," Sensors and Actuators A: Physical, vol. 132, pp. 376-384, 2006.
    [52] S. Muthukumar, et al., "Control of morphology and orientation of ZnO thin films grown on SiO2/Si substrates," Journal of Crystal Growth, vol. 225, pp. 197-201, 2001.
    [53] S.-Y. Chu, et al., "The investigation of preferred orientation growth of ZnO films on the PbTiO3-based ceramics and its application for SAW devices," Journal of Crystal Growth, vol. 257, pp. 280-285, 2003.
    [54] P. M. Martin, et al., "Piezoelectric films for 100-MHz ultrasonic transducers," Thin Solid Films, vol. 379, pp. 253-258, 2000.
    [55] Q. Chen, et al., "Property characterization of AlN thin films in composite resonator structure," Journal of Applied Physics, vol. 101, pp. 084103-8, 2007.
    [56] M. Eckert, "Theory from Wind Tunnels: Empirical Roots of Twentieth Century Fluid Dynamics," Centaurus, vol. 50, pp. 233-253, 2008.
    [57] I. Tani, "History of Boundary Layer Theory," Annual Review of Fluid Mechanics, vol. 9, pp. 87-111, 1977.
    [58] J. F. Clarke, "Gas dynamics with relaxation effects," Reports on Progress in Physics, vol. 41, pp. 807-864, 1978.
    [59] C. G. Elles and F. F. Crim, "CONNECTING CHEMICAL DYNAMICS IN GASES AND LIQUIDS," Annual Review of Physical Chemistry, vol. 57, pp. 273-302, 2006.
    [60] J. H. B. Smith, "Vortex Flows in Aerodynamics," Annual Review of Fluid Mechanics, vol. 18, pp. 221-242, 1986.
    [61] J. M. Wallace and P. V. Vukoslav?evi?, "Measurement of the Velocity Gradient Tensor in Turbulent Flows," Annual Review of Fluid Mechanics, vol. 42, pp. 157-181, 2010.
    [62] Z. Zhang, et al., "Pressure-driven flow in parallel-plate nanochannels," Applied Physics Letters, vol. 95, p. 154101, 2009.
    [63] Y.-H. Wang, et al., "MEMS-based gas flow sensors," Microfluidics and Nanofluidics, vol. 6, pp. 333-346, 2009.
    [64] G. Comte-Bellot, "Hot-Wire Anemometry," Annual Review of Fluid Mechanics, vol. 8, pp. 209-231, 1976.
    [65] Y. Wang, et al., "MEMS-based gas flow sensors," Microfluidics and Nanofluidics, vol. 6, pp. 333-346, 2009.
    [66] S. T. Wereley and C. D. Meinhart, "Recent Advances in Micro-Particle Image Velocimetry," Annual Review of Fluid Mechanics, vol. 42, pp. 557-576, 2010.
    [67] N. T. Nguyen, "Micromachined flow sensors--a review," Flow Measurement and Instrumentation, vol. 8, pp. 7-16, 1997.
    [68] K. L?nge, et al., "Surface acoustic wave biosensors: a review," Analytical and Bioanalytical Chemistry, vol. 391, pp. 1509-1519, 2008.
    [69] B. L. Yu, et al., "A micro channel integrated gas flow sensor for high sensitivity," in 11th Ieee Intersociety Conference on Thermal and Thermomechanical Phenomena in Electronic Systems, Vols 1-3, ed New York: Ieee, 2008, pp. 215-220.
    [70] I. Kao, et al., "Smart MEMS flow sensor: theoretical analysis and experimental characterization," IEEE sensors journal, vol. 7, pp. 713-722, 2007.
    [71] S. D. Holland and D. E. Chimenti, "Air-coupled acoustic imaging with zero-group-velocity Lamb modes," Applied Physics Letters, vol. 83, pp. 2704-2706, 2003.
    [72] C. Prada, et al., "Laser-based ultrasonic generation and detection of zero-group velocity Lamb waves in thin plates," Applied Physics Letters, vol. 87, pp. 194109-3, 2005.
    [73] A. A. Maznev and A. G. Every, "Surface acoustic waves with negative group velocity in a thin film structure on silicon," Applied Physics Letters, vol. 95, pp. 011903-3, 2009.
    [74] B. A. Martin, et al., "Viscosity and density sensing with ultrasonic plate waves," Sensors and Actuators A: Physical, vol. 22, pp. 704-708, 1989.
    [75] I. Viktorov, Rayleigh and Lamb Waves: Plenum, New York, 1967.
    [76] P. Lloyd and M. Redwood, "Wave propagation in a layered plate composed of two solids with perfect contact, slip, or a fluid layer at their interface," Acustica, vol. 16, pp. 224-232, 1965.
    [77] J. Achenbach, Wave propagation in elastic solids, 1973.
    [78] A. Bernard, et al., "Guided waves energy velocity in absorbing and non-absorbing plates," The Journal of the Acoustical Society of America, vol. 110, pp. 186-196, 2001.
    [79] M. Castaings and B. Hosten, "Guided waves propagating in sandwich structures made of anisotropic, viscoelastic, composite materials," The Journal of the Acoustical Society of America, vol. 113, pp. 2622-2634, 2003.
    [80] F. Mesa and D. Jackson, "Investigation of integration paths in the spectral-domain analysis of leaky modes on printed circuit lines," IEEE Transactions on Microwave Theory and Techniques, vol. 50, pp. 2267-2275, 2002.
    [81] N. T. Nguyen and R. M. White, "Acoustic streaming in micromachined flexural plate wave devices: numerical simulation and experimental verification," IEEE Trans Ultrason Ferroelectr Freq Control, vol. 47, pp. 1463-71, 2000.
    [82] T. Laurent, ""Generation, propagation et detection d' ondes de lamb. Modelisation et application aux membranes comportant des couches minces piezoelectriques sur silicium"," Ph.D., Department of electronic, University of Franche-Comté, Besancon, 1997.
    [83] R. Duhamel, "Study the biochemical sensor base on Lamb waves," Ph.D., Department of electronic, University of Franche-Comté, Besancon, 2005.
    [84] F. Li, "INNOVATIVE DETECTION METHODS IN LIQUID FOR A LAMB WAVE BIOSENSOR," Ph.D., Department of electronic, University of Franche-Comté, Besancon, 2008.
    [85] M. Deng and J. Pei, "Assessment of accumulated fatigue damage in solid plates using nonlinear Lamb wave approach," Applied Physics Letters, vol. 90, pp. 121902-3, 2007.
    [86] F. Lefevre, et al., "Laser ultrasonics and neural networks for the characterization of thin isotropic plates," Review of Scientific Instruments, vol. 80, pp. 014901-6, 2009.
    [87] Y.-C. Lee and S. H. Kuo, "Fluid dielectric loading on leaky Lamb wave of a piezoelectric plate," Applied Physics Letters, vol. 89, pp. 031920-3, 2006.
    [88] T. Rossing, Springer handbook of acoustics: Springer Verlag, 2007.
    [89] L. Zhou, et al., "Influence of gases on Lamb waves propagations in resonator," Applied Physics Letters, vol. 95, pp. 223505-3, 2009.
    [90] L. Brekhovskikh and V. Goncharov, Mechanics of continua and wave dynamics vol. 1. Berlin: Springer-verlag, 1985.
    [91] J. D. N. Cheeke, Fundamentals and applications of ultrasonic waves. Boca Raton: CRC Press, 2002.
    [92] C. Neto, et al., "Boundary slip in Newtonian liquids: a review of experimental studies," Reports on Progress in Physics, vol. 68, pp. 2859-2897, 2005.
    [93] H. E. Hager, "Fluid property evaluation by piezoelectric crystals operating in the thickness shear mode," Chemical Engineering Communications, vol. 43, pp. 25 - 38, 1986.
    [94] J. Kondoh and S. Shiokawa, "Measurements of conductivity and pH of liquid using surface acoustic wave devices," Jpn. J. Appl. Phys, vol. 31, pp. 82-84, 1992.
    [95] O.-W. Lau, et al., "Evaluation of methods to minimize effects of liquid viscosity and density on the oscillating frequencies of thickness-shear-mode (TSM) piezoelectric resonators," Analytica Chimica Acta, vol. 312, pp. 217-222, 1995.
    [96] S. J. Martin, et al., "Characterization of SH acoustic plate mode liquid sensors," Sensors and Actuators, vol. 20, pp. 253-268, 1989.
    [97] G. Kovacs, et al., "A love wave sensor for (bio)chemical sensing in liquids," Sensors and Actuators A: Physical, vol. 43, pp. 38-43, 1994.
    [98] F. Herrmann, et al., "Separate determination of liquid density and viscosity with sagittally corrugated Love-mode sensors," Sensors and Actuators A: Physical, vol. 78, pp. 99-107, 1999.
    [99] A. P. Sarvazyan, "Ultrasonic velocimetry of biological compounds," Annual Review of Biophysics and Biophysical Chemistry, vol. 20, pp. 321-42, 1991.
    [100] N. Doy, et al., "Small volume laboratory on a chip measurements incorporating the quartz crystal microbalance to measure the viscosity-density product of room temperature ionic liquids," Biomicrofluidics, vol. 4, p. 7, Mar 2010.
    [101] V. Raimbault, et al., "Molecular weight influence study of aqueous poly(ethylene glycol) solutions with a microfluidic Love wave sensor," Sensors and Actuators B: Chemical, vol. 144, pp. 318-322, 2010.
    [102] K. Mitsakakis, et al., "Parametric study of SH-SAW device response to various types of surface perturbations," Sensors and Actuators B: Chemical, vol. 138, pp. 408-416, 2009.
    [103] E. B. Freyer, "Sonic studies of the physical properties of liquids. II. The velocity of sound in solutions of certain alkali halides and their compressibilities," Journal of the American Chemical Society, vol. 53, pp. 1313-1320, 1931.
    [104] R. M. White and S. W. Wenzel, "Fluid loading of a Lamb-wave sensor," Applied Physics Letters, vol. 52, pp. 1653-1655, 1988.
    [105] Z. Chen, et al., "Separate determination of liquid properties with lamb wave devices," presented at the Proceedings of the 2006 IEEE International Frequency Control Symposium and Exposition, Vols 1 and 2, New York, 2006.
    [106] R. M. Moroney, et al., "Microtransport induced by ultrasonic Lamb waves," Applied Physics Letters, vol. 59, pp. 774-776, 1991.
    [107] A. Amararene, et al., "Water Confined in Reverse Micelles: Acoustic and Densimetric Studies," Journal of Physical Chemistry B, vol. 101, pp. 10751-10756, 1997.
    [108] B. N?lting, "Relation between adiabatic and pseudoadiabatic compressibility in ultrasonic velocimetry," Journal of Theoretical Biology, vol. 175, pp. 191-196, 1995.
    [109] P. C. Ho, et al., "Electrical conductivity measurements of aqueous sodium chloride solutions to 600°C and 300 MPa," Journal of Solution Chemistry, vol. 23, pp. 997-1018, 1994.
    [110] S. Adachi, Handbook on physical properties of semiconductors: Kluwer Academic Pub, 2004.
    [111] H. J. McSkimin and J. P. Andreatch, "Elastic Moduli of Silicon vs Hydrostatic Pressure at 25.0[degree]C and - 195.8[degree]C," Journal of Applied Physics, vol. 35, pp. 2161-2165, 1964.
    [112] V. I. Dimitrova, et al., "Study of reactive DC magnetron sputtering deposition of AlN thin films," Vacuum, vol. 49, pp. 193-197, 1998.
    [113] O. Ambacher, "Growth and applications of Group III-nitrides," Journal of Physics D: Applied Physics, vol. 31, p. 2653, 1998.
    [114] W. Chiu, "The Optical Properties and Applications of AlN Thin Film " Master, Chung Yuan Christian University, 2002.

© 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