Roy Olson Iii

Roy Olson Iii


Research Focus & Metrics

Academic Career Length

20Years (2007-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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12 November 2012 in MRS Bulletin
Verified
Journal Article
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GPGianluca Piazza
Gianluca Piazza
VFValeriy Felmetsger
Valeriy Felmetsger
Paul MuraltPaul Muralt
Paul Muralt
RIRoy Olson Iii
Roy Olson Iii
RRRichard Ruby
Richard Ruby

1 May 2007
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Conference Paper
Closed access
RIRoy Olson Iii
Roy Olson Iii
JFJames G. Fleming
James G. Fleming
KWKenneth E. Wojciechowski
Kenneth E. Wojciechowski
MBMichael S. Baker
Michael S. Baker
MTMelanie R. Tuck
Melanie R. Tuck
This paper reports post-CMOS compatible aluminum nitride (AlN) MEMS resonators, filters, and resonant sensors for the miniaturization of radio-frequency transceivers and sensor systems. Utilizing a resonator with two closely spaced modes, 2nd order MEMS filters occupying 0.06 mm2 have been realized in a single device. Methods for tuning the bandwidth and center frequency of these filters lithographically have been demonstrated. A 0.5% bandwidth, 108.4 MHz dual mode filter has a measured insertion loss of 9.4 dB with 50 Omega termination which can be reduced to 4.7 dB by terminating the filter with 75 Omega. In order to scale MEMS resonators to higher frequencies without increasing the size or impedance, resonators selectively driven at a harmonic determined by interdigitated drive and sense electrodes have been demonstrated reaching frequencies of 796 MHz with impedances of approximately 100 Omega and quality factors in excess of 750 in air. In the same process resonant sensors based on AlN double-ended tuning fork (DETF) sensing beams have been demonstrated at 727 kHz with quality factors of 2160. An oscillator based on the DETF sensing beams achieves a phase noise of -81 dBc/Hz at 275 Hz offset from the carrier. A 100 ng mass coupled to a pair of DETF sensors achieves an acceleration sensitivity of 565 mG/radicHz for accelerations from 275 to 1100 Hz.

1 January 2007
Verified
Conference Paper
Closed access
RIRoy Olson Iii
Roy Olson Iii
JFJames G. Fleming
James G. Fleming
IEIhab F. El-Kady
Ihab F. El-Kady
MTMelanie R. Tuck
Melanie R. Tuck
FMFrederick B. McCormick
Frederick B. McCormick
A MEMS bulk wave acoustic bandgap has been designed and experimentally verified. The acoustic bandgaps are realized by including tungsten (W) scatterers in a SiO2 matrix. Wide frequency ranges where acoustic waves are forbidden to exist are formed due to the large density and acoustic impedance mismatch between W and SiO2. The acoustic bandgap structures are fabricated in a 7-mask process that features integrated aluminum nitride piezoelectric couplers. Acoustic bandgaps in a square lattice have been measured at 33 and 67 MHz with up to 35 dB of acoustic rejection and bandwidths exceeding 35% of the midgap.

1 May 2007
Verified
Conference Paper
Closed access
RIRoy Olson Iii
Roy Olson Iii
BKBianca E. N. Keeler
Bianca E. N. Keeler
DCDavid A. Czaplewski
David A. Czaplewski
DCDustin W. Carr
Dustin W. Carr
This paper reports a MEMS displacement sensor with a sensitivity of 50 fm/radicHz at frequencies as low as 10 mHz. The sensor is composed of a near-field optical nano-grating that modulates the reflectivity of incident light by 10%/nm. A reference detection low noise readout circuit has been designed that cancels laser relative intensity noise (RIN) to frequencies as low as 0.7 Hz. The low frequency bandwidth of the position sensing microsystem is further reduced to below 10 mHz using a new MEMS correlated double sampling technique that cancels low frequency RIN, drift, and circuit 1/f noise by greater than 77 dB.