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Please use this identifier to cite or link to this item: http://hdl.handle.net/10012/6575

Title: Magnetic Transduction for RF Micromechanical Filters
Authors: Forouzanfar, Sepehr
Keywords: Lorentz force
transduction
micromechanical
resonator
filter
MEMS
electrodynamic
RF
Approved Date: 27-Feb-2012
Date Submitted: 21-Feb-2012
Abstract: The use of electrostatic transduction has enabled high-Q miniaturized mechanical resonators made of non-piezoelectric material that vibrate at high and ultra high frequencies. However, this transduction technique suffers from large values of motional resistance associated with the technique, limiting its use for interfacing to standard 50 RF circuits. Piezoelectric transduction has advantages over the electrostatic method because of its comparable to 50 motional resistance. However, the technique requires use of thin film piezoelectric materials with the demonstrated Qs that are much lower than their corresponding non-piezoelectric resonators. This research proposes use of electrodynamic transduction, reports analytic and experimental studies on electrodynamic transduction for RF application, highlights the method’s advantages, and lists the contributions. The use of Lorentz-force transduction for RF micromechanical filters proposed in this work is pursued by experimentally evaluating the transduction technique implemented for microfabricated designs. By fabricating single and coupled microresonators in a few different fabrication technologies, including CMOS35, the performance of the Lorentz-force driven microresonators is studied. Using a laser vibrometer, the actual performance, including the displacement and velocity of the moving points of the microstructures’ surfaces, are measured. The mode shapes and resonance specifications of the microstructures in air and vacuum derived by laser vibrometer provide data for characterizing the employed Lorentz-force transduction technique. Furthermore, the results from the electrical measurements are compared to the micromechanical resonators’ frequency response obtained from the mechanical measurements by laser vibrometer. The significantly low values of motional resistance computed for the differently fabricated designs demonstrate the advantage of Lorentz-force transduction for RF filter applications. Should a device similar in size be driven electrostatically, the motional resistance would be multiple orders of magnitude higher. This research reports the experimental results obtained by examining a Lorentz- force transduction application for developing RF micromechanical filters. The results demonstrate the Lorentz-force transduction’s advantages over other transduction methods used for RF μ-mechanical filters. Compared to electrostatic transduction, the Lorentz-force method provides greater electromechanical coupling, multiple orders of magnitude lower motional resistance, the independence of the filter center frequency from the bias voltage, higher power handling, and no requirement for bias lines, which decreases the work in microfabrication. Unlike piezoelectric transduction, the electrodynamic technique requires no piezoelectric material. Use of non-piezoelectric materials provides more flexibility for resonator material in the IC-compatible fabrications. Power handling in electrodynamic transduction has fewer limitations than other transduction techniques because the higher power needed in electrostatic or piezoelectric methods requires a higher voltage, which is limited by the breakdown voltage. The higher power in Lorentz-force-based transduction demands a larger current. The larger current produces heat that is removable by applying an appropriate cooling technique.
Program: Electrical and Computer Engineering
Department: Electrical and Computer Engineering
Degree: Doctor of Philosophy
URI: http://hdl.handle.net/10012/6575
Appears in Collections:Faculty of Engineering Theses and Dissertations
Electronic Theses and Dissertations (UW)

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Forouzanfar_Sepehr.pdfThesis14.38 MBAdobe PDFView/Open
DThirdModeInphase2.aviElectrodynamically driven CMOS35 coupled three resonator16.42 MBaviView/Open
DThirdModeInphase1.aviElectrodynamically driven CMOS35 coupled three resonator12.67 MBaviView/Open
DFirstModeOutphase9.aviElectrodynamically driven CMOS35 coupled three resonator14.99 MBaviView/Open
DFirstModeOutphase8.aviElectrodynamically driven CMOS35 coupled three resonator15.11 MBaviView/Open
DFirstModeOutphase7.aviElectrodynamically driven CMOS35 coupled three resonator10.5 MBaviView/Open
DFirstModeOutphase6.aviElectrodynamically driven CMOS35 coupled three resonator19.24 MBaviView/Open
DFirstModeOutphase5.aviElectrodynamically driven CMOS35 coupled three resonator16.44 MBaviView/Open
DFirstModeOutphase4.aviElectrodynamically driven CMOS35 coupled three resonator12.67 MBaviView/Open
DFirstModeOutphase3.aviElectrodynamically driven CMOS35 coupled three resonator15.11 MBaviView/Open
DFirstModeOutphase2.aviElectrodynamically driven CMOS35 coupled three resonator8.36 MBaviView/Open
DFirstModeInphase5.aviElectrodynamically driven CMOS35 coupled three resonator14.99 MBaviView/Open
DFirstModeInphase3.aviElectrodynamically driven CMOS35 coupled three resonator10.77 MBaviView/Open
DFirstModeInOutphse1.aviElectrodynamically driven CMOS35 coupled three resonator14.99 MBaviView/Open
CoupUWQuartOutphase1.aviElectrodynamically driven UW-MEMS coupled two resonator8.7 MBaviView/Open
CoupUWQuartInphase1.aviElectrodynamically driven UW-MEMS coupled two resonator10.51 MBaviView/Open
CoupUWMEMSQuartOutphase1.aviElectrodynamically driven UW-MEMS coupled two resonator13.26 MBaviView/Open
CoupUWMEMS598KHzOutphase1stMode.aviElectrodynamically driven UW-MEMS coupled two resonator14.82 MBaviView/Open
CoupUWMEMSQuartInphase1.aviElectrodynamically driven UW-MEMS coupled two resonator11.83 MBaviView/Open
CoupUWMEMS476KHzInphase1stMode.aviElectrodynamically driven UW-MEMS coupled two resonator14.81 MBaviView/Open
CoupledUWMEMShigherMode1.aviElectrodynamically driven UW-MEMS coupled two resonator10.86 MBaviView/Open
BFirstModeOutphase2.aviElectrodynamically driven CMOS35 coupled two resonator13.77 MBaviView/Open
BFirstModeInphase2.aviElectrodynamically driven CMOS35 coupled two resonator13.77 MBaviView/Open
AThirdModeOutphase2.aviElectrodynamically driven CMOS35 coupled two resonator14.72 MBaviView/Open
AThirdmodeInphase2.aviElectrodynamically driven CMOS35 coupled two resonator14.72 MBaviView/Open
AFirstModeOutphase3.aviElectrodynamically driven CMOS35 coupled two resonator10.08 MBaviView/Open
AFirstModeInphase3.aviElectrodynamically driven CMOS35 coupled two resonator10.08 MBaviView/Open
U2ThirdmodeVac1.aviElectrodynamically driven single resonator17.67 MBaviView/Open
U2ThirdmodeAir1.aviElectrodynamically driven single resonator16.41 MBaviView/Open
U2Thirdmode1.aviElectrodynamically driven single resonator14.88 MBaviView/Open
U2FifthmodeVac1.aviElectrodynamically driven single resonator17.67 MBaviView/Open
U2FifthMode1.aviElectrodynamically driven single resonator17.67 MBaviView/Open
U1FirstModeAir1.aviElectrodynamically driven single resonator16.87 MBaviView/Open
PFirstMode1.aviElectrodynamically driven single resonator16.47 MBaviView/Open
CFirstModeAir1.aviElectrodynamically driven single resonator15.41 MBaviView/Open


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