Please use this identifier to cite or link to this item: https://doi.org/10.1063/1.1448888
DC FieldValue
dc.titleGap state distribution in amorphous hydrogenated silicon carbide films deduced from photothermal deflection spectroscopy
dc.contributor.authorChew, K.
dc.contributor.authorRusli
dc.contributor.authorYoon, S.F.
dc.contributor.authorAhn, J.
dc.contributor.authorZhang, Q.
dc.contributor.authorLigatchev, V.
dc.contributor.authorTeo, E.J.
dc.contributor.authorOsipowicz, T.
dc.contributor.authorWatt, F.
dc.date.accessioned2014-10-16T08:29:27Z
dc.date.available2014-10-16T08:29:27Z
dc.date.issued2002-04-01
dc.identifier.citationChew, K., Rusli, Yoon, S.F., Ahn, J., Zhang, Q., Ligatchev, V., Teo, E.J., Osipowicz, T., Watt, F. (2002-04-01). Gap state distribution in amorphous hydrogenated silicon carbide films deduced from photothermal deflection spectroscopy. Journal of Applied Physics 91 (7) : 4319-4325. ScholarBank@NUS Repository. https://doi.org/10.1063/1.1448888
dc.identifier.issn00218979
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/93875
dc.description.abstractThe density of gap states distribution in silicon (Si) rich hydrogenated amorphous silicon carbide (a-Si 1-xC x:H) films with varying carbon (C) fraction (x) is investigated by the photothermal deflection spectroscopy (PDS). The films are grown using the Electron Cyclotron Resonance Chemical Vapor Deposition (ECR-CVD) technique. By using different methane-to-silane gas flow ratios, a-Si 1-xC x:H with x ranging from 0 to 0.36 are obtained. A deconvolution procedure is performed based on a proposed DOS model for these Si rich a-Si 1-xC x:H. Good fits between the simulated and experimental spectra are achieved, thus rendering support to the model proposed. Deduction of the DOS enables us to obtain various parameters, including the optical gap and the valence band tail width. The fitted mobility gap E g is found to be well correlated to the Tauc gap E tauc and E 04 gap deduced from the optical absorption spectra. A correlation is also seen between the fitted valence band tail width E vu, the Urbach energy E u and the defect density. All these parameters are seen to increase with C alloying. A shift in the defect energy level in the midgap with increasing C incorporation is observed, together with a broadening of the defect distribution and a stronger correlation between the defect bands, which can be accounted for in terms of the influence of C dangling bonds on the deep defect density distribution. © 2002 American Institute of Physics. © 2002 American Institute of Physics.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1063/1.1448888
dc.sourceScopus
dc.typeArticle
dc.contributor.departmentPHYSICS
dc.contributor.departmentCHEMISTRY
dc.description.doi10.1063/1.1448888
dc.description.sourcetitleJournal of Applied Physics
dc.description.volume91
dc.description.issue7
dc.description.page4319-4325
dc.description.codenJAPIA
dc.identifier.isiut000174663900056
Appears in Collections:Staff Publications

Show simple item record
Files in This Item:
There are no files associated with this item.

Google ScholarTM

Check

Altmetric


Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.