RF-MEMS load sensors with enhanced Q-factor and sensitivity in a suspended architecture

buir.contributor.authorDemir, Hilmi Volkan
buir.contributor.orcidDemir, Hilmi Volkan|0000-0003-1793-112X
dc.citation.epage253en_US
dc.citation.issueNumber3en_US
dc.citation.spage247en_US
dc.citation.volumeNumber88en_US
dc.contributor.authorMelik, R.en_US
dc.contributor.authorUnal, E.en_US
dc.contributor.authorPerkgoz, N. K.en_US
dc.contributor.authorPuttlitz, C.en_US
dc.contributor.authorDemir, Hilmi Volkanen_US
dc.date.accessioned2016-02-08T09:54:04Z
dc.date.available2016-02-08T09:54:04Z
dc.date.issued2010-11-09en_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentDepartment of Physicsen_US
dc.departmentNanotechnology Research Center (NANOTAM)en_US
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)en_US
dc.description.abstractIn this paper, we present and demonstrate RF-MEMS load sensors designed and fabricated in a suspended architecture that increases their quality-factor (Q-factor), accompanied with an increased resonance frequency shift under load. The suspended architecture is obtained by removing silicon under the sensor. We compare two sensors that consist of 195 μm × 195 μm resonators, where all of the resonator features are of equal dimensions, but one's substrate is partially removed (suspended architecture) and the other's is not (planar architecture). The single suspended device has a resonance of 15.18 GHz with 102.06 Q-factor whereas the single planar device has the resonance at 15.01 GHz and an associated Q-factor of 93.81. For the single planar device, we measured a resonance frequency shift of 430 MHz with 3920 N of applied load, while we achieved a 780 MHz frequency shift in the single suspended device. In the planar triplet configuration (with three devices placed side by side on the same chip, with the two outmost ones serving as the receiver and the transmitter), we observed a 220 MHz frequency shift with 3920 N of applied load while we obtained a 340 MHz frequency shift in the suspended triplet device with 3920 N load applied. Thus, the single planar device exhibited a sensitivity level of 0.1097 MHz/N while the single suspended device led to an improved sensitivity of 0.1990 MHz/N. Similarly, with the planar triplet device having a sensitivity of 0.0561 MHz/N, the suspended triplet device yielded an enhanced sensitivity of 0.0867 MHz/N.en_US
dc.description.provenanceMade available in DSpace on 2016-02-08T09:54:04Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2011en
dc.identifier.doi10.1016/j.mee.2010.10.041en_US
dc.identifier.issn0167-9317
dc.identifier.urihttp://hdl.handle.net/11693/21998
dc.language.isoEnglishen_US
dc.publisherElsevieren_US
dc.relation.isversionofhttp://dx.doi.org/10.1016/j.mee.20http://dx.doi.org/10.10.041en_US
dc.source.titleMicroelectronic Engineeringen_US
dc.subjectBio-implanten_US
dc.subjectFabricationen_US
dc.subjectICen_US
dc.subjectQuality-factoren_US
dc.subjectResonance frequency shiften_US
dc.subjectRF-MEMSen_US
dc.subjectNatural frequenciesen_US
dc.subjectPower inductorsen_US
dc.subjectQ factor measurementen_US
dc.subjectResonatorsen_US
dc.subjectSensorsen_US
dc.subjectFrequency shift keyingen_US
dc.titleRF-MEMS load sensors with enhanced Q-factor and sensitivity in a suspended architectureen_US
dc.typeArticleen_US

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