Transition metal oxides on organic semiconductors
buir.contributor.author | Demir, Hilmi Volkan | |
buir.contributor.orcid | Demir, Hilmi Volkan|0000-0003-1793-112X | |
dc.citation.epage | 877 | en_US |
dc.citation.issueNumber | 4 | en_US |
dc.citation.spage | 871 | en_US |
dc.citation.volumeNumber | 15 | en_US |
dc.contributor.author | Zhao Y. | en_US |
dc.contributor.author | Zhang, J. | en_US |
dc.contributor.author | Liu, S. | en_US |
dc.contributor.author | Gao, Y. | en_US |
dc.contributor.author | Yang, X. | en_US |
dc.contributor.author | Leck K.S. | en_US |
dc.contributor.author | Abiyasa, A. P. | en_US |
dc.contributor.author | Divayana, Y. | en_US |
dc.contributor.author | Mutlugun, E. | en_US |
dc.contributor.author | Tan S.T. | en_US |
dc.contributor.author | Xiong, Q. | en_US |
dc.contributor.author | Demir, Hilmi Volkan | en_US |
dc.contributor.author | Sun, X. W. | en_US |
dc.date.accessioned | 2015-07-28T12:03:19Z | |
dc.date.available | 2015-07-28T12:03:19Z | |
dc.date.issued | 2014-04 | en_US |
dc.department | Department of Physics | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.description.abstract | Transition metal oxides (TMOs) on organic semiconductors (OSs) structure has been widely used in inverted organic optoelectronic devices, including inverted organic light-emitting diodes (OLEDs) and inverted organic solar cells (OSCs), which can improve the stability of such devices as a result of improved protection of air sensitive cathode. However, most of these reports are focused on the anode modification effect of TMO and the nature of TMO-on-OS is not fully understood. Here we show that the OS on TMO forms a two-layer structure, where the interface mixing is minimized, while for TMO-on-OS, due to the obvious diffusion of TMO into the OS, a doping-layer structure is formed. This is evidenced by a series of optical and electrical studies. By studying the TMO diffusion depth in different OS, we found that this process is governed by the thermal property of the OS. The TMO tends to diffuse deeper into the OS with a lower evaporation temperature. It is shown that the TMO can diffuse more than 20 nm into the OS, depending on the thermal property of the OS. We also show that the TMO-on-OS structure can replace the commonly used OS with TMO doping structure, which is a big step toward in simplifying the fabrication process of the organic optoelectronic devices. (C) 2014 Elsevier B.V. All rights reserved. | en_US |
dc.description.provenance | Made available in DSpace on 2015-07-28T12:03:19Z (GMT). No. of bitstreams: 1 HV21.pdf: 1396479 bytes, checksum: 23f68d6ace953b4011c4ae9b5ba2e628 (MD5) | en |
dc.identifier.doi | 10.1016/j.orgel.2014.01.011 | en_US |
dc.identifier.issn | 1566-1199 | |
dc.identifier.uri | http://hdl.handle.net/11693/12832 | |
dc.language.iso | English | en_US |
dc.publisher | Elsevier BV | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1016/j.orgel.2014.01.011 | en_US |
dc.source.title | Organic Electronics: materials, physics, chemistry and applications | en_US |
dc.subject | Transition metal oxide | en_US |
dc.subject | Organic semiconductor | en_US |
dc.subject | Diffusion | en_US |
dc.subject | Organic light-emitting diode | en_US |
dc.subject | P-doping | en_US |
dc.title | Transition metal oxides on organic semiconductors | en_US |
dc.type | Article | en_US |
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