<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-04-17T05:57:48Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2117/87190" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2117/87190</identifier><datestamp>2026-02-04T03:34:50Z</datestamp><setSpec>com_2072_1033</setSpec><setSpec>col_2072_452950</setSpec></header><metadata><oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
   <dc:title>A thickness-shear MEMS resonator employing electromechanical transduction through a coplanar waveguide</dc:title>
   <dc:creator>Johnson, W.L.</dc:creator>
   <dc:creator>Wallis, T.M.</dc:creator>
   <dc:creator>Kabos, P.</dc:creator>
   <dc:creator>Rocas Cantenys, Eduard</dc:creator>
   <dc:creator>Collado Gómez, Juan Carlos</dc:creator>
   <dc:creator>Liew, L.A.</dc:creator>
   <dc:creator>Ha, J.Y.</dc:creator>
   <dc:creator>Davydov, A.V.</dc:creator>
   <dc:creator>Plankis, A.</dc:creator>
   <dc:creator>Heyliger, P.R.</dc:creator>
   <dc:contributor>Universitat Politècnica de Catalunya. Departament de Teoria del Senyal i Comunicacions</dc:contributor>
   <dc:contributor>Universitat Politècnica de Catalunya. CSC - Components and Systems for Communications Research Group</dc:contributor>
   <dc:subject>Microelectromechanical systems</dc:subject>
   <dc:subject>Acoustic power</dc:subject>
   <dc:subject>Acoustic resonance</dc:subject>
   <dc:subject>Electromechanical transduction</dc:subject>
   <dc:subject>Fabricated device</dc:subject>
   <dc:subject>Finite-element</dc:subject>
   <dc:subject>High damping</dc:subject>
   <dc:subject>MEMS resonators</dc:subject>
   <dc:subject>Noise levels</dc:subject>
   <dc:subject>Non-Linearity</dc:subject>
   <dc:subject>Nulling</dc:subject>
   <dc:subject>Orders of magnitude</dc:subject>
   <dc:subject>Out-of-plane displacement</dc:subject>
   <dc:subject>Reference lines</dc:subject>
   <dc:subject>Shear displacement</dc:subject>
   <dc:subject>Silicon-bridge</dc:subject>
   <dc:subject>SOI wafers</dc:subject>
   <dc:subject>Swept-frequency</dc:subject>
   <dc:subject>Thermoelastic damping</dc:subject>
   <dc:subject>Thickness-shear</dc:subject>
   <dc:subject>Vibrational trapping</dc:subject>
   <dc:subject>Waveguide thickness</dc:subject>
   <dc:subject>Sistemes microelectromecànics</dc:subject>
   <dc:description>The design, modeling, fabrication, and characterization&#xd;
of a vibrationally trapped thickness-shear MEMS resonator&#xd;
is presented. This device is intended to avoid various limitations&#xd;
of flexural MEMS resonators, including nonlinearity, clamping&#xd;
losses, thermoelastic damping, and high damping in liquid. It&#xd;
includes a silicon bridge and a reference line on an SOI wafer,&#xd;
a coupled Au/Cr coplanar waveguide, Lorentz-force coupling,&#xd;
variations in waveguide thickness for vibrational trapping, and&#xd;
circuitry for nulling the components of the signal that are&#xd;
unrelated to the acoustic resonance. Finite-element vibrational&#xd;
modeling shows the lowest thickness-shear mode with a bridge&#xd;
thickness of 4.9 µm to be dominated by shear displacements,&#xd;
with the magnitude of out-of-plane displacements decreasing with&#xd;
increasing bridge width. Two-dimensional modeling of vibrational&#xd;
trapping, with central regions of the waveguides having&#xd;
43 nm greater thickness, indicates that amplitudes are reduced&#xd;
by several orders of magnitude at the ends of the bridges for&#xd;
the fundamental ~ 400 MHz thickness-shear resonance. Sweptfrequency&#xd;
network-analyzer measurements of fabricated devices&#xd;
reveal no evidence for an acoustic resonance, despite a calculated&#xd;
prediction of levels of acoustic power absorption that are well&#xd;
above the measured noise level. A possible explanation for this&#xd;
result is stiction of the bridges to the substrate.</dc:description>
   <dc:description>Peer Reviewed</dc:description>
   <dc:description>Postprint (published version)</dc:description>
   <dc:date>2012</dc:date>
   <dc:type>Conference report</dc:type>
   <dc:identifier>Johnson, W., Wallis, T., Kabos, P., Rocas, E., Collado, J., Liew, L., Ha, J., Davydov, A., Plankis, A., Heyliger, P. A thickness-shear MEMS resonator employing electromechanical transduction through a coplanar waveguide. A: IEEE Frequency Control Symposium. "2012 IEEE International Frequency Control Symposium, IFCS 2012, Proceedings". 2012, p. 452-457.</dc:identifier>
   <dc:identifier>978-145771819-9</dc:identifier>
   <dc:identifier>https://hdl.handle.net/2117/87190</dc:identifier>
   <dc:identifier>10.1109/FCS.2012.6243722</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:rights>Restricted access - publisher's policy</dc:rights>
   <dc:format>6 p.</dc:format>
   <dc:format>application/pdf</dc:format>
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