Please use this identifier to cite or link to this item: https://doi.org/10.1088/1742-6596/34/1/134
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dc.titleProcess analysis and optimization on PECVD amorphous silicon on glass substrate
dc.contributor.authorOng, Y.Y.
dc.contributor.authorChen, B.T.
dc.contributor.authorTay, F.E.H.
dc.contributor.authorIliescu, C.
dc.date.accessioned2014-06-17T06:31:39Z
dc.date.available2014-06-17T06:31:39Z
dc.date.issued2006-04-01
dc.identifier.citationOng, Y.Y., Chen, B.T., Tay, F.E.H., Iliescu, C. (2006-04-01). Process analysis and optimization on PECVD amorphous silicon on glass substrate. Journal of Physics: Conference Series 34 (1) : 812-817. ScholarBank@NUS Repository. https://doi.org/10.1088/1742-6596/34/1/134
dc.identifier.issn17426588
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/61152
dc.description.abstractIn this paper, depositing of low stress Amorphous Silicon (α-Si) with high deposition rate by using a plasma-enhanced chemical vapour deposition (PECVD) system (STS, Multiplex Pro-CVD) was studied. The influence of the process parameters, such as power, frequency mode, argon flow rate, temperature and pressure, on these objectives have been studied and optimized. RF modes (13.56 MHz and 380 kHz) have obvious influence on the deposition rate of amorphous silicon, which revealed that high RF mode provide higher deposition rate, but not certain on the residue stress. The power has a proportional relationship to the deposition rate, and also, is proportional to stress induced at high RF mode, so low power is preferred for low stress film. At high RF mode, the deposition rate decreases with temperature while stress increases. By increasing the gas flow rate of argon, the film stress is found to decrease for both RF modes, while the deposition rate decreases for the low RF mode. Lastly, at high RF mode, pressure is also proportional to deposition rate and stress (compressive). The proper process conditions were optimized to get the low stress α-Si. The application of -α-Si sacrificial layer in the glass etching process is also briefly highlighted and illustrated at the end of this paper. © 2006 IOP Publishing Ltd.
dc.sourceScopus
dc.subjectAmorphous silicon
dc.subjectDeposition rate
dc.subjectLow stress
dc.subjectPECVD
dc.typeArticle
dc.contributor.departmentMECHANICAL ENGINEERING
dc.description.doi10.1088/1742-6596/34/1/134
dc.description.sourcetitleJournal of Physics: Conference Series
dc.description.volume34
dc.description.issue1
dc.description.page812-817
dc.identifier.isiut000286667100134
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