Frequency-dependent piezoresistive effect in top-down fabricated gold nanoresistors
buir.contributor.author | Hanay, Mehmet Selim | |
buir.contributor.orcid | Hanay, Mehmet Selim|0000-0002-1928-044X | |
dc.citation.epage | 6539 | en_US |
dc.citation.issueNumber | 15 | en_US |
dc.citation.spage | 6533 | en_US |
dc.citation.volumeNumber | 21 | en_US |
dc.contributor.author | Arı, A. B. | |
dc.contributor.author | Karakan, M. Ç. | |
dc.contributor.author | Yanık, C. | |
dc.contributor.author | Kaya, İ. İ. | |
dc.contributor.author | Hanay, Mehmet Selim | |
dc.contributor.author | Svitelskiy, O. | |
dc.contributor.author | González, M. | |
dc.contributor.author | Seren, H. | |
dc.contributor.author | Ekinci, K. L. | |
dc.date.accessioned | 2022-01-26T12:50:38Z | |
dc.date.available | 2022-01-26T12:50:38Z | |
dc.date.issued | 2021-08-11 | |
dc.department | Department of Mechanical Engineering | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.description.abstract | Piezoresistive strain gauges allow for electronic readout of mechanical deformations with high fidelity. As piezoresistive strain gauges are aggressively being scaled down for applications in nanotechnology, it has become critical to investigate their physical attributes at different limits. Here, we describe an experimental approach for studying the piezoresistive gauge factor of a gold thin-film nanoresistor as a function of frequency. The nanoresistor is fabricated lithographically near the anchor of a nanomechanical doubly clamped beam resonator. As the resonator is driven to resonance in one of its normal modes, the nanoresistor is exposed to frequency-dependent strains of ε ≲ 10–5 in the 4–36 MHz range. We calibrate the strain using optical interferometry and measure the resistance changes using a radio frequency mix-down technique. The piezoresistive gauge factor γ of our lithographic gold nanoresistors is γ ≈ 3.6 at 4 MHz, in agreement with comparable macroscopic thin metal film resistors in previous works. However, our γ values increase monotonically with frequency and reach γ ≈ 15 at 36 MHz. We discuss possible physics that may give rise to this unexpected frequency dependence. | en_US |
dc.description.provenance | Submitted by Mustafa Er (mer@bilkent.edu.tr) on 2022-01-26T12:50:37Z No. of bitstreams: 1 Frequency-dependent_piezoresistive_effect_in_top-down_fabricated_gold_nanoresistors.pdf: 3760494 bytes, checksum: 916200ea88d165e4fd6fcaf15877f987 (MD5) | en |
dc.description.provenance | Made available in DSpace on 2022-01-26T12:50:38Z (GMT). No. of bitstreams: 1 Frequency-dependent_piezoresistive_effect_in_top-down_fabricated_gold_nanoresistors.pdf: 3760494 bytes, checksum: 916200ea88d165e4fd6fcaf15877f987 (MD5) Previous issue date: 2021-08-11 | en |
dc.identifier.doi | 10.1021/acs.nanolett.1c01733 | en_US |
dc.identifier.eissn | 1530-6992 | |
dc.identifier.issn | 1530-6984 | |
dc.identifier.uri | http://hdl.handle.net/11693/76807 | |
dc.language.iso | English | en_US |
dc.publisher | American Chemical Society | en_US |
dc.relation.isversionof | https://doi.org/10.1021/acs.nanolett.1c01733 | en_US |
dc.source.title | Nano Letters | en_US |
dc.subject | Piezoresistive effect | en_US |
dc.subject | Piezoresistive gauge factor | en_US |
dc.subject | Gold nanowire | en_US |
dc.subject | Gold nanoresistor | en_US |
dc.subject | NEMS | en_US |
dc.title | Frequency-dependent piezoresistive effect in top-down fabricated gold nanoresistors | en_US |
dc.type | Article | en_US |
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