001     151846
005     20240708133645.0
024 7 _ |a 10.1139/cjp-2013-0604
|2 doi
024 7 _ |a 1208-6045
|2 ISSN
024 7 _ |a 0008-4204
|2 ISSN
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037 _ _ |a FZJ-2014-01704
082 _ _ |a 530
100 1 _ |a Grootoonk, B.
|0 P:(DE-Juel1)140348
|b 0
245 _ _ |a Monitoring of powder formation via optical emission spectroscopy and self-bias-voltage measurements for high depletion µc-Si:H deposition regimes
260 _ _ |a Ottawa, Ontario
|c 2014
|b NCR Research Press
336 7 _ |a Journal Article
|b journal
|m journal
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|s 1420633533_23891
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336 7 _ |a Output Types/Journal article
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336 7 _ |a ARTICLE
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336 7 _ |a JOURNAL_ARTICLE
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336 7 _ |a article
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520 _ _ |a Microcrystalline silicon fabricated by plasma-enhanced chemical vapour deposition (PECVD) is commonly used as an absorber material in thin-film tandem solar cells. The source gases used in the μc-Si:H PECVD process are silane and hydrogen. One way to further increase the production efficiency of solar modules is to increase the gas utilization during deposition of the silicon absorber layer. In this work this is achieved by reducing the hydrogen flow. These deposition conditions are known to promote powder formation in the plasma, which can be detrimental for the solar cell’s conversion efficiency as well as for the maintenance of the system. Therefore, an easily applicable approach to determine powder formation in-situ during the PECVD process is presented. Both the self-bias-voltage and the ratio of the optical emissions from SiH* to Hβ as function of the gas residence time in the plasma is used to determine the onset of powder formation. Furthermore, a clear link between the precursor gas residence time in the plasma to the onset of powder formation is shown independent of the chosen pressure.
536 _ _ |a 111 - Thin Film Photovoltaics (POF2-111)
|0 G:(DE-HGF)POF2-111
|c POF2-111
|f POF II
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536 _ _ |0 G:(DE-Juel1)HITEC-20170406
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|c HITEC-20170406
|a HITEC - Helmholtz Interdisciplinary Doctoral Training in Energy and Climate Research (HITEC) (HITEC-20170406)
588 _ _ |a Dataset connected to CrossRef, juser.fz-juelich.de
700 1 _ |a Woerdenweber, J.
|0 P:(DE-HGF)0
|b 1
700 1 _ |a Gordijn, A.
|0 P:(DE-Juel1)130242
|b 2
700 1 _ |a Gabriel, O.
|0 P:(DE-HGF)0
|b 3
700 1 _ |a Meier, Matthias
|0 P:(DE-Juel1)130830
|b 4
|u fzj
773 _ _ |a 10.1139/cjp-2013-0604
|g Vol. 92, no. 7/8, p. 736 - 739
|0 PERI:(DE-600)2021497-2
|n 7/8
|p 736 - 739
|t Canadian journal of physics
|v 92
|y 2014
|x 1208-6045
909 C O |o oai:juser.fz-juelich.de:151846
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910 1 _ |a Forschungszentrum Jülich GmbH
|0 I:(DE-588b)5008462-8
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910 1 _ |a Forschungszentrum Jülich GmbH
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910 1 _ |a Forschungszentrum Jülich GmbH
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913 2 _ |a DE-HGF
|b Forschungsbereich Energie
|l Erneuerbare Energien
|1 G:(DE-HGF)POF3-120
|0 G:(DE-HGF)POF3-121
|2 G:(DE-HGF)POF3-100
|v Solar cells of the next generation
|x 0
913 1 _ |a DE-HGF
|b Energie
|l Erneuerbare Energien
|1 G:(DE-HGF)POF2-110
|0 G:(DE-HGF)POF2-111
|2 G:(DE-HGF)POF2-100
|v Thin Film Photovoltaics
|x 0
|4 G:(DE-HGF)POF
|3 G:(DE-HGF)POF2
914 1 _ |y 2014
915 _ _ |a Peer review unknown
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981 _ _ |a I:(DE-Juel1)IMD-3-20101013


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