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Haskell, Reichl B. "A Surface Acoustic Wave Mercury Vapor Sensor". Fogler Library, University of Maine, 2003. http://www.library.umaine.edu/theses/pdf/HaskellRB2003.pdf.
Pełny tekst źródłaHong, Stanley Seokjong 1977. "Surface acoustic wave optical modulation". Thesis, Massachusetts Institute of Technology, 2001. http://hdl.handle.net/1721.1/86715.
Pełny tekst źródłaIncludes bibliographical references (leaves 50-54).
by Stanley Seokjong Hong.
M.Eng.
Hay, Robert Russell. "Digitally-tunable surface acoustic wave resonator". [Boise, Idaho] : Boise State University, 2009. http://scholarworks.boisestate.edu/td/58/.
Pełny tekst źródłaMcNeil, Robert Peter Gordon. "Surface acoustic wave quantum electronic devices". Thesis, University of Cambridge, 2012. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.610718.
Pełny tekst źródłaKaplan, Emrah. "Surface acoustic wave enhanced electroanalytical sensors". Thesis, University of Glasgow, 2015. http://theses.gla.ac.uk/6557/.
Pełny tekst źródłaKenny, Thomas Donald. "Identification of High-Velocity Pseudo-surface Acoustic Wave Substrate Orientations and Modeling of Surface Acoustic Wave Structures". Fogler Library, University of Maine, 2011. http://www.library.umaine.edu/theses/pdf/KennyT2011.pdf.
Pełny tekst źródłaBanerjee, Markus K. "Acoustic wave interactions with viscous liquids spreading in the acoustic path of a surface acoustic wave sensor". Thesis, Nottingham Trent University, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.302521.
Pełny tekst źródłaThorn, Adam Leslie. "Electron dynamics in surface acoustic wave devices". Thesis, University of Cambridge, 2009. https://www.repository.cam.ac.uk/handle/1810/224176.
Pełny tekst źródłaAstley, Michael Robert. "Surface-acoustic-wave-defined dynamic quantum dots". Thesis, University of Cambridge, 2008. https://www.repository.cam.ac.uk/handle/1810/261973.
Pełny tekst źródłaDu, X. "Surface acoustic wave devices for microfluidic applications". Thesis, University of Cambridge, 2009. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.598662.
Pełny tekst źródłaGell, Jennifer Rachel. "Surface-acoustic-wave (SAW) driven light sources". Thesis, University of Cambridge, 2008. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.599350.
Pełny tekst źródłaSehra, Gurmukh S. "Surface acoustic wave based flavour sensor system". Thesis, University of Warwick, 2004. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.416148.
Pełny tekst źródłaMeng, Qingbin. "Surface acoustic wave controlled semiconductor optical source". Thesis, University of Bath, 2009. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.518122.
Pełny tekst źródłaThe FISOS is analyzed as two sub-divisions, optical source and acoustic processor, which have the common substrate structure. The optical beams excited from the optical source part of the device undergoes a scattering in the Bragg grating formed by SAWs that are generated by an IDT positioned on top of the acoustic processing part of device. By altering the property (power, frequency, etc.) of the SAW, versatile functionalities such as modulation, filtering, beam steering and so on of the optical beams can be realized in this optical source device.
A multilayer structure based on GaN/InGaN MQWs grown on sapphire is designed for the FISOS to be blue light emitting and efficiently launching SAWs. An etch-down technique employed in the SAW processing part is taken to improve the overlap between the optical and acoustic waves and then the interaction efficiency. Optimizations to the geometrical dimensions of the FISOS, such the width of the ridge waveguide, the position of the IDT and the etching depth, etc., are discussed in the given structure.
Numerical models are investigated to access the operational characteristics and then to provide design guidelines for the proposed integrated device. The Bragg diffraction of optical waves occurring within the acoustic waves in the proposed structure are simulated as a two-dimensional interaction between two guided optical modes and an acoustic surface wave.
The modal distributions and propagation velocities of SAWs in a multilayer system are calculated using Adler’s matrix method. The electrical characteristics of an IDT, such as impedance, insertion loss, electromechanical constant and so on are also discussed.
Transverse and lateral optical modes in the given multilayer structure are analyzed by the transfer matrix method. The interaction of optical waves and acoustic waves are modeled using the rigorous grating diffraction theory. Starting from Floquet’s theory, the well-known coupled-wave method and modal method can both be derived from the rigorous grating diffraction theory. Discussions of some useful approximate methods are also presented. In this thesis, the simulations of the acoustooptic interaction are performed using the coupled-wave method.
From the simulation results, the angular distribution profile and spatial profile of the output of the FISOS are evaluated. An improvement to the expression of the diffraction efficiency in such an integrated device is proposed. The so-called beam diffraction efficiency gives a more complete measure to the acoustooptic diffraction and is used to investigate the features of FISOS different from conventional acoustooptic devices. Contour plots of the beam efficiency varying with acoustic frequency and power in a FISOS is demonstrated to be a convenient and powerful approach in the device design.
The operational performances of an integrated deflector and a modulator in FISOS are analyzed to investigate the feasibility of FISOS. The trade-off of the efficiency-resolution in an integrated deflector design is discussed. Short interaction length, high acoustic frequency and narrow ridge are proved to be helpful for a larger number of resolvable spots with a fairly high efficiency. In the case of the integrated modulator, given that the figure of merit Q is fixed, it is demonstrated that the smaller the Q, the longer the interaction length, larger ridge width and lower acoustic frequency will give rise to a larger bandwidth, though the highest efficiency might appear at a higher frequency.
Some practical issues such as the misalignment of planar elements on the device and the incoherence of the integrated optical source are also discussed. A modified working frequency can be used to compensate the efficiency loss in the former case; in the latter case, it is demonstrated that a distortion of beam diffraction efficiency versus acoustic power with an incoherent optical source arises due to the wide spectrum of the incident optical waves.
Gizeli, Electra. "New acoustic wave sensor geometries". Thesis, University of Cambridge, 1992. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.282004.
Pełny tekst źródłaBright, Victor M. "Shear horizontal surface acoustic waves". Diss., Georgia Institute of Technology, 1992. http://hdl.handle.net/1853/14831.
Pełny tekst źródłaKitabayashi, Hiroyuki. "Surface acoustic wave filters on diamond layered structures /". *McMaster only, 2001.
Znajdź pełny tekst źródłaAlghane, Mansuor Mohamed. "Surface acoustic wave streaming in a microfluidic system". Thesis, Heriot-Watt University, 2013. http://hdl.handle.net/10399/2645.
Pełny tekst źródłaKhalid, Muhammad Arslan. "Engineering surface acoustic wave sensing and diagnostic devices". Thesis, University of Glasgow, 2017. http://theses.gla.ac.uk/30999/.
Pełny tekst źródłaFriedlander, Jeffrey B. "Wireless Strain Measurement with Surface Acoustic Wave Sensors". The Ohio State University, 2011. http://rave.ohiolink.edu/etdc/view?acc_num=osu1306874020.
Pełny tekst źródłaChiu, Ching-Sang Denner Warren W. "Report on the Office of Naval Research USA-China Conference on Shallow Water Acoustics, December 18-21, 1995". Monterey, CA : Naval Postgraduate School, 1997. http://catalog.hathitrust.org/api/volumes/oclc/37486128.html.
Pełny tekst źródłaReese, Owein. "Homogenization of acoustic wave propagation in a magnetorheological fluid". Link to electronic thesis, 2004. http://www.wpi.edu/Pubs/ETD/Available/etd-0430104-101629.
Pełny tekst źródłaSen, Rahul. "Acoustic scattering by discontinuities in waveguides". Diss., Virginia Polytechnic Institute and State University, 1988. http://hdl.handle.net/10919/81021.
Pełny tekst źródłaPh. D.
Kavalov, Dimitar A. "Surface acoustic wave neural networks for RF signal processing". Thesis, Oxford Brookes University, 2002. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.249406.
Pełny tekst źródłaNash, Geoffrey Richard. "Surface acoustic wave investigations of low dimensional electron systems". Thesis, University of Bath, 1996. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.320474.
Pełny tekst źródłaTew, R. "Imaging theory of surface-breaking discontinuities". Thesis, University of Oxford, 1987. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.380008.
Pełny tekst źródłaSrinivasan, krishnan. "Nanomaterial sensing layer based surface acoustic wave hydrogen sensors". [Tampa, Fla.] : University of South Florida, 2005. http://purl.fcla.edu/fcla/etd/SFE0001325.
Pełny tekst źródłaTran, Tuan A. "Extrinsic Fabry-Perot interferometer for surface acoustic wave measurement". Thesis, This resource online, 1991. http://scholar.lib.vt.edu/theses/available/etd-10242009-020318/.
Pełny tekst źródłaBlaess, Guido. "Häusung von Surface-acoustic-wave-Sensoren für die Bioanalytik". Karlsruhe : Forschungszentrum Karlsruhe, 2006. http://d-nb.info/983159173/34.
Pełny tekst źródłaSchuler, Leo Pius. "Wireless identification and sensing using surface acoustic wave devices". Thesis, University of Canterbury. Electrical Engineering, 2003. http://hdl.handle.net/10092/1081.
Pełny tekst źródłaSchuler, Leo P. "Wireless identification and sensing using surface acoustic wave devices". Thesis, University of Canterbury. Engineering, 2003. http://hdl.handle.net/10092/8565.
Pełny tekst źródłaGates, Michael Richard. "Surface acoustic wave investigations of spin and pseudospin systems". Thesis, University of Nottingham, 2002. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.247121.
Pełny tekst źródłaRimsa, Roberts. "Surface acoustic wave microfluidic pumps for on-chip diagnostics". Thesis, University of Leeds, 2018. http://etheses.whiterose.ac.uk/22524/.
Pełny tekst źródłaMiller, James Henry 1957. "Estimation of sea surface wave spectra using acoustic tomography". Thesis, Massachusetts Institute of Technology, 1987. http://hdl.handle.net/1721.1/44595.
Pełny tekst źródłaBibliography: p. 164-171.
Vita.
by James Henry Miller.
Sc.D.
Srinivasan, Krishnan. "Nanomaterial Sensing Layer Based Surface Acoustic Wave Hydrogen Sensors". Scholar Commons, 2005. https://scholarcommons.usf.edu/etd/873.
Pełny tekst źródłaKim, Yoonkee. "Surface acoustic wave propagation in multilayered and multichannel waveguide structures". Diss., Georgia Institute of Technology, 1993. http://hdl.handle.net/1853/15060.
Pełny tekst źródłaFurnell, G. D. "A study of acoustic wave propagation within curved ducting systems /". Title page, table of contents and abstract only, 1989. http://web4.library.adelaide.edu.au/theses/09PH/09phf987.pdf.
Pełny tekst źródłaBerry, David Leonard. "Acoustic scattering by near-surface inhomogeneities in porous media". Thesis, Open University, 1990. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.254021.
Pełny tekst źródłaJohari, Houri. "Micromachined capacitive silicon bulk acoustic wave gyroscopes". Diss., Atlanta, Ga. : Georgia Institute of Technology, 2008. http://hdl.handle.net/1853/31656.
Pełny tekst źródłaCommittee Chair: Dr. Farrokh Ayazi; Committee Co-Chair: Dr. F. Levant Degertekin; Committee Member: Dr. Paul Kohl; Committee Member: Dr. Peter Hesketh; Committee Member: Dr. Suresh K. Sitaraman. Part of the SMARTech Electronic Thesis and Dissertation Collection.
RUIZ, ALBERTO. "SURFACE ACOUSTIC WAVE VELOCITY MEASUREMENTS ON SURFACE-TREATED METALS BY LASER-ULTRASONIC SPECTROSCOPY". University of Cincinnati / OhioLINK, 2004. http://rave.ohiolink.edu/etdc/view?acc_num=ucin1077302192.
Pełny tekst źródłaParmar, Biren Jagadish. "Development Of Point-Contact Surface Acoustic Wave Based Sensor System". Thesis, Indian Institute of Science, 2006. https://etd.iisc.ac.in/handle/2005/279.
Pełny tekst źródłaLin, Xin-Yu, i 林信宇. "Composite Surface Acoustic Wave Substrate". Thesis, 2009. http://ndltd.ncl.edu.tw/handle/80342744786128229150.
Pełny tekst źródła正修科技大學
電子工程研究所
98
The (100) oriented Aluminum nitrogen (AlN) thin films have excellent bulk acoustic wave (BAW) and surface acoustic wave (SAW) properties. In this study, the piezoelectric 64°-YX LiNbO3 substrate was used to fabricate the SAW devices. We also deposited (100) oriented AlN thin film on this lithium niobate (LiNbO3) substrate to form a new composite substrate (AlN/LiNbO3) using reactive radio frequency magnetron sputtering method. The SAW devices were fabricated on the composite substrate and the effects of AlN film thickness on the composite substrate properties have been investigated. The SAW interdigital transducer electrodes were deposited on the top of those substrates by the sputtering and photolithography methods in the process. The network analyzer was used to measure the center frequency and electromechanical coupling coefficient (K2) of the SAW devices. The spectrum analyzer was used to estimate the temperature coefficient of frequency (TCF). The SAW filter fabricated by the LiNbO3 substrate showed the center frequency, TCF and K2 are 45.66 MHz, -62.49 ppm/℃ and 11.07%, respectively. On the other hand, the SAW filter fabricated by the composite substrate with AlN film thickness is 0.5 μm. It is found that center frequency, TCF and K2 are 46.13 MHz, -58.62 ppm/℃ and 9.79%, respectively. When the composite substrate with 1 μm-thickness AlN film, the SAW filter showed the center frequency, TCF and K2 are 46.22MHz, -53.41 ppm/℃ and 7.21%, respectively. The experimented results showed the center frequency, TCF and K2 are 46.39 MHz, -50.11 ppm/℃ and 6.54%, respectively. In this study, AlN thin films were successfully prepared on the LiNbO3 substrate by reactive RF magnetron sputtering method. The results exhibited the composite substrate can increase the SAW velocity, and improve the temperature coefficient of frequency.
Chiu, Shih-Chuan, i 邱仕釧. "Design of Surface Acoustic Wave Gyroscope". Thesis, 2005. http://ndltd.ncl.edu.tw/handle/5wt3wa.
Pełny tekst źródła國立交通大學
機械工程系所
93
The preliminary design and performance evaluation of a radio frequency MEMS gyroscope, based on a surface acoustic wave resonator (SAWR) and a surface acoustic wave sensor (SAWS) is presented in this work. In addition, the method to convert the transmitted power into exact particle displacement is introduced to predict the sensing resolution of this MEMS gyroscope. Microelectromechanical systems (MEMS) sensors have received more attention over the last decade. They generally have the advantages of being lightweight, small in size, low power consumption and low cost, due to standard IC fabrication techniques. The gyroscopes, operated on the surface acoustic wave, are expected to have a better performance limitations over current MEMS vibratory gyroscope designs, for example, low cost, better robustness and reliability.
Young, Ming-Sheng, i 楊明昇. "Characteristics of Surface Acoustic Wave Sensor". Thesis, 2001. http://ndltd.ncl.edu.tw/handle/81672173386487190179.
Pełny tekst źródła國立成功大學
電機工程學系
89
This paper is primarily divided into two sections. In section 1, the design and fabrication of IF SAW device are described. In section 2, the sensing property of SAW gas sensor for ethanol vapor is discussed. Based on sensing requirement, the first condition for SAW device design is low insertion loss that promising whole oscillation circuit can work normally. We choose LiNbO3 to be substrate and construct grating reflectors. The insertion loss of SAW device with 30 pairs grating reflections is 4 ~ 4.5dB, and that with 50 pairs grating reflectors is about 3.5dB. By using mass loading effect, SAW device may regard as ethanol vapor density sensor. The response due to changes in the medium density on the SAW transmission path causes transmission velocity change and resonant frequency shift. This is the basic principle of a SAW gas sensor. In order to increase sensitivity, coating stearic acid as sensing film on the transmission path is used. For different film depth, we discuss the responses of resonant frequency shift and find out the optimum. At last, the improvements of sensor system, range and stability are given.
Wang, Bing-Yu, i 王炳昱. "2.45GHz Surface Acoustic Wave RFID device". Thesis, 2012. http://ndltd.ncl.edu.tw/handle/04739017499281301108.
Pełny tekst źródła國立中興大學
機械工程學系所
100
Currently, surface acoustic radio frequency identification (SAW RFID) tag received increasing attention because of several advantages such as large reliable reading range, low power consumptions, able to operate high temperature range from -40C to 400C and able to be used in harsh environment. One pair of metallic interdigital transducers (IDT) and several reflectors are on the surface of SAW tags. When an electrical signal is applied to IDT, a mechanical acoustic wave will be triggered and transferred to reflector. The time-dependent reflection waves return to IDT, and mechanical waves retransform to AC signals through direct piezoelectric effect. When different patterns of AC signals are measured and recorded, different individual tags will be identified. For SAW RFID tags, the central frequency and number of possible codes are two of most important parameters. In this study, SAW RFID device were operated in high harmonic modes at 2.45GHz. Moreover, encoding scheme was studied to increase the information capacity of SAW tags. In this thesis, the 2.45GHz center frequency of Surface Acoustic Waves Radio Frequency Identification (SAW RFID) tag was developed. The substrate of SAW RFID was 128°Y-X cut Lithium Niobate (LiNbO3) piezoelectric substrate. The width of the IDT and reflectors were designed as 400nm to achieve center frequency of SAW tag as 2.45 GHz. The time position encoding and phase encoding were used to enhance the information capacity of SAW tags. The IDT and reflectors were deposited on the LiNbO3 piezoelectric substrate successfully by E-beam lithography and lift-off technique.
Pu, Rui Zhen, i 蒲瑞臻. "Study of Diamond Surface Acoustic Wave Filter". Thesis, 2003. http://ndltd.ncl.edu.tw/handle/73906707995566481528.
Pełny tekst źródła國立臺北科技大學
材料及資源工程系碩士班
91
This study have focused on three parts of the diamond surface acoustic wave(SAW)filter, including ultrasonic pulse experiment of material, make smooth diamond thin film, and deposition ZnO thin film. Diamond film and oriented ZnO thin film can be used in high frequency, high power and good temperature stability of SAW filters. Materials study for diamond SAW filter is the objective in this study. First, the elastic properties of materials are determined by ultrasonic pulse experiment. The effects of crystal structure and elastic constant or the acoustic wave echo velocity, in different direction structure and under various acoustic wave, were determined. Results indicated that longitudinal wave velocities in (111) direction of diamond single crystal and diamond thick film are the fastest. The two steps elastic modulus equation derived from elastic modulus, Young’s modulus (1223Gpa) and Bulk modulus (481Gpa), confirmed that (111) face in diamond have the fastest wave velocities. Second, this study investigated the application of diamond thin film by HF-CVD method. The system pressure and CH4/H2 flow rates were fixed in this experiment. The effects of the hot filament distance (15mm, 10mm) and the substrate temperature(700℃, 900℃)on the dimond thin film were performed in order to obtain high flateness and low roughness. The results showed that increasing substrate temperature results in low nucleation, which leads to a large graim and better crystallinality. The average surface roughness(Ra)is 7nm. When the substrate temperature is lower the nucleation is high, which nesults in a smaller grain size and poor crystallinality. The average surface roughness(Ra)is 3nm. Third, this study investigated the ZnO thin film prepared by RF magnetron sputter. Oiriented (002) ZnO thin film was successfully deposited on glass substrate. The results indicated the process parameters(RF power, the ratio of oxygen/argon mass flow)affect the thin film characteristics such as deposition rate, grain size and grain orientation. The optimal conditions for sputtering are 150W of RF power and 1/2 of oxygen/argon mass flow ratio. Under such circumstance, the deposition rate of the film was 0.8μm/hr, and a (002) C-axis oriented columnar grain structure of ZnO film was formed.
Nian, Yi-Wei, i 粘益維. "Optimal Design of Surface Acoustic Wave Devices". Thesis, 2014. http://ndltd.ncl.edu.tw/handle/5hk358.
Pełny tekst źródła國立臺南大學
材料科學系碩士班
102
This studied plan is to propose an innovated process for fabricating the flexible SAW devices by sol-gel technology and fully ink jet technology. The ZnO solution is prepared by sol-gel technology. We design inter digital transducer (IDT) pattern and deposits ZnO solution on the flexible polyimide plastic (PI) substrate by fully ink jet process. Next, the frequency of SAW device can be measured by the function generator and spectrum analyzer. Here, 7.2MHz is the maximum gain of this device, it will be observed as the SAW center operating frequency. Through the comparison between the predicted value and experimental center frequency, the experimental center frequencies agree with the predicted value. The analysis of surface acoustic wave propagation characteristics is processed by the Finite Element Method (FEM).To discuss various designed parameters affect the central frequency response,and the numerical model will be built for optimization. The electrode thickness is reduced from 1um to 0.5um,and the frequency is raised from 7.2MHz to 7.8MHz . I simulate aluminum nitride (AlN) as piezoelectric materials and the electrode thickness is reduced from 1um to 0.5um,and the frequency is raised from 13.4MHz to 13.9MHz.
Feng, Yi-Shuo, i 馮顗碩. "A New-Type Surface Acoustic Wave Filter". Thesis, 2014. http://ndltd.ncl.edu.tw/handle/88178144542455205846.
Pełny tekst źródła國立臺灣大學
機械工程學研究所
102
This thesis proposed that if we bond a piezoelectric material on substrate which deposited the electrodes and etched trenches between the electrodes, we can exclude mass and stiffness effect by IDTs (Inter digital transducers) on substrate. Through this method, we can let the SAW propagate on clean and flat piezoelectric material achieves more accurate filtering effect. This method not only eliminates the cost of trimming, but also provides the good protection ability to the filter. First, this thesis chose the ST-cut quartz piezoelectric as material to transfer SAW, and used Z-cut quartz as bottom substrate and build IDTs on its top. Then we etched a trench between the IDTs. Last of all we used SU8-1040 to bond ST-cut quartz and Z-cut quartz together. Through the above method we successfully manufacture a two ports SAW filter by ST-cut quartz. The electrode period is 88μm and the theoretical value of center frequency is 35.8773MHz. The center frequency of the filter with the theoretical error only one-thousandth, and the surface of wave propagation is between two wafers, it will let the filter hermetic packaged directly. By eliminating the step of trimming and extra package, we can develop a low-cost and small SAW filters.
Chiu, Chun-HO, i 邱俊豪. "A New-Type Surface Acoustic Wave Filter". Thesis, 2013. http://ndltd.ncl.edu.tw/handle/01521144110049783333.
Pełny tekst źródła國立臺灣大學
機械工程學研究所
101
It is proposed that the saw(surface acoustic wave) propagation characteristics in a half–space piezoelectric crystal will change as the depth or duty cycle ratio of the periodic electrodes is tuned. Considering the saw propagation in half-space piezoelectric crystal with periodic electrodes, which are conductors and have mass and stiffness, periodic electrodes affect the saw propagation with the three reasons. Mass and stiffness effects belong to mechanical effects, while being conductors affecting the electric potential of the substrate belongs to electric effects. The behavior of a piezoelectric crystal can be expressed by constitutive equations. Besides, displacement and electric field in a periodic structure are expressed by Floquet Theorem. A general form of saw propagation in a half-space piezoelectric substrate can be expressed by solving the wave equations. The homogeneous solution can be solved by a periodic BVP(boundary value problem), including periodic boundary conditions and electrical boundary conditions. An alternative voltage is given as the input to the IDT(interdigital transducer) in the derivation of the actuator. By the methods described above, the frequency response can be obtained. The frequency corresponding to the peak in the frequency response plot can be tuned by adjusting the depth or duty cycle ratio of the electrodes. The filter part is placed between two transducers, which are one actuator and one receiver. The wavelength of the saw fits the period of the electrode in the filter, so only saw meeting the periodic boundary condition exists. And one can change the selected frequency by adjusting the depth or duty cycle ratio of the electrodes. In the derivation of the saw receiver, the concept of impedance matching is applied. Assumed there is a saw that makes the electric potential difference of the IDT to be 1 volt. The charge density is obtained by integrating electric displacement. And the current can be derived by taking time derivative on the charge density. The impedance can be easily shown by the ratio of voltage difference to the current. The three parts and a pair of extra reflectors are synthesized to be the saw device. All these parts can be adjusted by tuning the depth or duty cycle ratio of the electrodes. Moreover, when it comes to the yield, tuning the duty cycle ratio is preferred due to its easier way in fabrications than tuning the depth.
Chen, Han-Jan, i 陳漢珍. "An Integrable Surface Acoustic Wave Notch Filter". Thesis, 2002. http://ndltd.ncl.edu.tw/handle/41093301022907822665.
Pełny tekst źródła國立成功大學
微電子工程研究所碩博士班
90
Although Surface Acoustic Wave Notch Filter was investigated in the past, the structures of these devices often needed the extra lumped-element : resistance R、capacitance C and inductance L so that the devices are complex and integrated hardly. From this, we offer a simple planar structure of the SAW notch filters that have smaller size and can be fabricated easily. It has several advantages such as easy-integrated; smaller size and no power dissipation. We adopt the interdigital transducers and delay line to fabricate the SAW notch filter. In this paper, we use an interdigital transducer finger width 8 mm with conventional photolithography process; lift-off technique; piezoelectric materials to fabricate on the 128° rotated YX-cut Lithium Niobate (LiNbO3). Finally, we get the frequency responses of the SAW notch filter: the center frequency 113.4 MHz; the 3dB bandwidth 0.36 %; the insertion loss S21= –10.583 dB.
Hung, Chia-hsun, i 洪嘉珣. "Study of Broadband Surface Acoustic Wave Antenna". Thesis, 2011. http://ndltd.ncl.edu.tw/handle/34683406321781827716.
Pełny tekst źródła國立臺南大學
電機工程研究所
99
In recent years, antenna developments have been fueled by the rapid development of modern wireless communication systems. In particular, communication products have become an indispensable part of people''s daily lives. An antenna plays the important role in communication systems as it has independent properties that affect the wireless radio frequency (RF) receiver as a whole. In the past, antennas have studied in radar and satellite equipment extensively, so the sizes are very large. Recent portable communication developments in the study of light-weight, compact, rugged, lower cost optical transmitters and receivers. A novel miniaturized broadband surface acoustic wave (SAW) antenna using interdigital transducers (IDTs) and microstrip structure is proposed. The antenna with size of 0.8×1×0.5 cm3 is designed on the piezoelectric materials to fabricate 128°rotated Y-cut lithium niobate (LiNbO3) piezoelectric substrate. The antenna is constructed using four cross-coupled half-wave length square open-loop strips and two 16-m-width interdigital transducers (IDTs) of 42 pairs, utilizing the semiconductor process including lithography and evaporation. The impedance bandwidth (S11 < -10 dB) is achieved over the frequency range from 4.8 to 7 GHz for WLAN/WiMAX bands. This proposed antenna with broadband matched impedance, low cost, easy to manufacture and compact size can be suitable for communication products of WLAN/WiMAX applications.