Please use this identifier to cite or link to this item: https://doi.org/10.1016/j.cap.2018.05.002
DC FieldValue
dc.titleEnergy level alignment of blended organic semiconductors and electrodes at the interface
dc.contributor.authorWhitcher, TJ
dc.contributor.authorWong, WS
dc.contributor.authorTalik, AN
dc.contributor.authorWoon, KL
dc.contributor.authorRusydi, A
dc.contributor.authorChanlek, N
dc.contributor.authorNakajima, H
dc.contributor.authorSaisopa, T
dc.contributor.authorSongsiriritthigul, P
dc.date.accessioned2019-06-03T04:40:12Z
dc.date.available2019-06-03T04:40:12Z
dc.date.issued2018-09-01
dc.identifier.citationWhitcher, TJ, Wong, WS, Talik, AN, Woon, KL, Rusydi, A, Chanlek, N, Nakajima, H, Saisopa, T, Songsiriritthigul, P (2018-09-01). Energy level alignment of blended organic semiconductors and electrodes at the interface. CURRENT APPLIED PHYSICS 18 (9) : 982-992. ScholarBank@NUS Repository. https://doi.org/10.1016/j.cap.2018.05.002
dc.identifier.issn15671739
dc.identifier.issn18781675
dc.identifier.urihttps://scholarbank.nus.edu.sg/handle/10635/155056
dc.description.abstract© 2018 Korean Physical Society The energy level alignment of a blended mixture of organic semiconductors is often depicted as having a common vacuum level. However, this is not a universal phenomenon among the vast number of organic semiconductors that currently exist, as in many cases the energy levels align via the Fermi level. In this report, the energy level alignments of the mixtures; poly(9-vinylcarbazole) (PVK) and 2,7-bis(diphenylphosphoryl)-9,9′-spirobifluorene (SPPO13) and poly(3-hexylthiophene-2,5-diyl) (P3HT) and SPPO13, with varying SPPO13 concentrations, are measured. It was found that the blended systems exhibit two different vacuum levels with the dipole between the PVK and SPPO13 increasing with the SPPO13 concentration, whilst the P3HT and SPPO13 vacuum levels only experience a small change. This is attributed to the decreasing electronic screening with increasing SPPO13 concentration. These new observations have an important implication in our understanding of interfacial behaviour for blended systems commonly used in various organic electronic devices.
dc.language.isoen
dc.publisherELSEVIER SCIENCE BV
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 International
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/
dc.sourceElements
dc.subjectScience & Technology
dc.subjectTechnology
dc.subjectPhysical Sciences
dc.subjectMaterials Science, Multidisciplinary
dc.subjectPhysics, Applied
dc.subjectMaterials Science
dc.subjectPhysics
dc.subjectEnergy level alignment
dc.subjectVacuum level
dc.subjectBlended organic semiconductors
dc.subjectHETEROJUNCTION SOLAR-CELLS
dc.subjectMETAL INTERFACES
dc.subjectBARRIER HEIGHTS
dc.subjectCHARGE-TRANSFER
dc.subjectLAYER
dc.subjectPOLY(3-HEXYLTHIOPHENE)
dc.subject1ST-PRINCIPLES
dc.subjectEFFICIENCY
dc.subjectPOLYMER
dc.subjectSURFACE
dc.typeArticle
dc.date.updated2019-06-03T01:49:18Z
dc.contributor.departmentCENTRE FOR ADVANCED 2D MATERIALS
dc.contributor.departmentPHYSICS
dc.description.doi10.1016/j.cap.2018.05.002
dc.description.sourcetitleCURRENT APPLIED PHYSICS
dc.description.volume18
dc.description.issue9
dc.description.page982-992
dc.published.statePublished
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