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BSAC Research Review Individual Project

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Implemented in standard FEA codes using a complex-valued change of coordinates. Effectively change properties smoothly for perfect matching of mechanical impedance ... – PowerPoint PPT presentation

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Title: BSAC Research Review Individual Project


1
Introduction
Perfectly Matched Layers
  • High frequency surface-micromachined MEMS
    resonators have many applications
  • Filters, frequency references, sensors
  • Need high quality factors
  • Difficult to predict analytically
  • Existing tools predict frequency, but not Q
  • Anchor loss is a major damping source
  • Simulate anchor loss with perfectly matched
    layers
  • Illustrate anchor loss in disk resonators
  • Predict surprising sensitivity to geometry
  • Assume waves from the anchor are not reflected
    (i.e. the substrate is semi-infinite).
  • Add damping at the boundaries to absorb waves
  • Implemented in standard FEA codes using a
    complex-valued change of coordinates
  • Effectively change properties smoothly for
    perfect matching of mechanical impedance

Basic Loss Mechanism
Model of a Disk Resonator
Device micrographs (top) and schematic (bottom)
Displacement and mean energy flux at resonance
  • Simulated and built poly-SiGe disk resonators
  • 31.5 and 41.5 micron radii, 1.5 micron height
  • Post is 1.5 micron radius, 1 microns height
  • Fabricated dimensions vary from nominal
  • Axisymmetric finite element model, bicubic
    elements with 0.25 micron node spacing
  • Dominant mode is not purely radial
  • Includes a small bending motion
  • Vertical motion at post pumps elastic waves into
    the substrate
  • More bending motion when radial and bending
    modes are close in frequency

Conclusions
Design Sensitivity
  • Anchor loss is complicated even for disks!
  • Surprising dips in Q from interacting modes
  • Poisson coupling is important acoustic
    approximations are inadequate
  • Need CAD tools to predict damping
  • Simulate wafer with a perfectly matched layer
  • Have integrated anchor loss and thermoelastic
    damping models into HiQLab simulator
  • http//www.cs.berkeley.edu/dbindel/hiqlab/

Simulated Q for two modes (solid lines, left) at
different film thicknesses matches lab
measurement (dots). The behavior is explained by
the interaction of two complex frequencies near a
critical geometry.
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