An all-ZnO microbolometer for infrared imaging
buir.contributor.author | Okyay, Ali Kemal | |
dc.citation.epage | 249 | en_US |
dc.citation.spage | 245 | en_US |
dc.citation.volumeNumber | 67 | en_US |
dc.contributor.author | Kesim, Y. E. | en_US |
dc.contributor.author | Battal, E. | en_US |
dc.contributor.author | Tanrikulu, M. Y. | en_US |
dc.contributor.author | Okyay, Ali Kemal | en_US |
dc.date.accessioned | 2016-02-08T11:00:31Z | |
dc.date.available | 2016-02-08T11:00:31Z | |
dc.date.issued | 2014 | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.department | Nanotechnology Research Center (NANOTAM) | en_US |
dc.description.abstract | Microbolometers are extensively used for uncooled infrared imaging applications. These imaging units generally employ vanadium oxide or amorphous silicon as the active layer and silicon nitride as the absorber layer. However, using different materials for active and absorber layers increases the fabrication and integration complexity of the pixel structure. In order to reduce fabrication steps and therefore increase the yield and reduce the cost of the imaging arrays, a single layer can be employed both as the absorber and the active material. In this paper, we propose an all-ZnO microbolometer, where atomic layer deposition grown zinc oxide is employed both as the absorber and the active material. Optical constants of ZnO are measured and fed into finite-difference-time-domain simulations where absorption performances of microbolometers with different gap size and ZnO film thicknesses are extracted. Using the results of these optical simulations, thermal simulations are conducted using finite-element-method in order to extract the noise equivalent temperature difference (NETD) and thermal time constant values of several bolometer structures with different gap sizes, arm and film thicknesses. It is shown that the maximum performance of 171 mK can be achieved with a body thickness of 1.1 μm and arm thickness of 50 nm, while the fastest response with a time constant of 0.32 ms can be achieved with a ZnO thickness of 150 nm both in arms and body. © 2014 Elsevier B.V. All rights reserved. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T11:00:31Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2014 | en |
dc.identifier.doi | 10.1016/j.infrared.2014.07.023 | en_US |
dc.identifier.issn | 1350-4495 | |
dc.identifier.uri | http://hdl.handle.net/11693/26486 | |
dc.language.iso | English | en_US |
dc.publisher | Elsevier BV | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1016/j.infrared.2014.07.023 | en_US |
dc.source.title | Infrared Physics & Technology | en_US |
dc.subject | Atomic layer deposition | en_US |
dc.subject | Microbolometers | en_US |
dc.subject | Transparent conductive oxides | en_US |
dc.subject | Uncooled infrared imaging | en_US |
dc.subject | Zinc oxide | en_US |
dc.title | An all-ZnO microbolometer for infrared imaging | en_US |
dc.type | Article | en_US |
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