Low power zinc-oxide based charge trapping memory with embedded silicon nanoparticles via poole-frenkel hole emission
buir.contributor.author | Okyay, Ali Kemal | |
dc.citation.epage | 013112-4 | en_US |
dc.citation.spage | 013112-1 | en_US |
dc.citation.volumeNumber | 104 | en_US |
dc.contributor.author | El-Atab, N. | en_US |
dc.contributor.author | Ozcan, A. | en_US |
dc.contributor.author | Alkis, S. | en_US |
dc.contributor.author | Okyay, Ali Kemal | en_US |
dc.contributor.author | Nayfeh, A. | en_US |
dc.date.accessioned | 2016-02-08T10:58:59Z | |
dc.date.available | 2016-02-08T10:58:59Z | |
dc.date.issued | 2014 | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.department | Nanotechnology Research Center (NANOTAM) | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.description.abstract | A low power zinc-oxide (ZnO) charge trapping memory with embedded silicon (Si) nanoparticles is demonstrated. The charge trapping layer is formed by spin coating 2 nm silicon nanoparticles between Atomic Layer Deposited ZnO steps. The threshold voltage shift (ΔVt) vs. programming voltage is studied with and without the silicon nanoparticles. Applying -1 V for 5 s at the gate of the memory with nanoparticles results in a ΔVt of 3.4 V, and the memory window can be up to 8 V with an excellent retention characteristic (>10 yr). Without nanoparticles, at -1 V programming voltage, the ΔVt is negligible. In order to get ΔVt of 3.4 V without nanoparticles, programming voltage in excess of 10 V is required. The negative voltage on the gate programs the memory indicating that holes are being trapped in the charge trapping layer. In addition, at 1 V the electric field across the 3.6 nm tunnel oxide is calculated to be 0.36 MV/cm, which is too small for significant tunneling. Moreover, the ΔVt vs. electric field across the tunnel oxide shows square root dependence at low fields (E 1 MV/cm) and a square dependence at higher fields (E > 2.7 MV/cm). This indicates that Poole-Frenkel Effect is the main mechanism for holes emission at low fields and Phonon Assisted Tunneling at higher fields. © 2014 AIP Publishing LLC. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T10:58:59Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2014 | en |
dc.identifier.doi | 10.1063/1.4861590 | en_US |
dc.identifier.issn | 0003-6951 | |
dc.identifier.uri | http://hdl.handle.net/11693/26376 | |
dc.language.iso | English | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1063/1.4861590 | en_US |
dc.source.title | Applied Physics Letters | en_US |
dc.subject | Atomic layer deposited | en_US |
dc.subject | Charge trapping layers | en_US |
dc.subject | Charge trapping memory | en_US |
dc.subject | Phonon assisted tunneling | en_US |
dc.subject | Retention characteristics | en_US |
dc.subject | Silicon nanoparticles | en_US |
dc.subject | Square-root dependence | en_US |
dc.subject | Threshold voltage shifts | en_US |
dc.subject | Atomic layer deposition | en_US |
dc.subject | Charge trapping | en_US |
dc.subject | Electric fields | en_US |
dc.subject | Silicon | en_US |
dc.subject | Zinc | en_US |
dc.subject | Zinc oxide | en_US |
dc.subject | Nanoparticles | en_US |
dc.title | Low power zinc-oxide based charge trapping memory with embedded silicon nanoparticles via poole-frenkel hole emission | en_US |
dc.type | Article | en_US |
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