001     57973
005     20240708133629.0
024 7 _ |2 DOI
|a 10.1016/j.tsf.2005.08.282
024 7 _ |2 WOS
|a WOS:000234124700054
024 7 _ |a altmetric:21817592
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037 _ _ |a PreJuSER-57973
041 _ _ |a eng
082 _ _ |a 070
084 _ _ |2 WoS
|a Materials Science, Multidisciplinary
084 _ _ |2 WoS
|a Materials Science, Coatings & Films
084 _ _ |2 WoS
|a Physics, Applied
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |a Qiao, Z.
|b 0
|0 P:(DE-HGF)0
245 _ _ |a Dielectric modeling of transmittance spectra of thin ZnO:Al films
260 _ _ |a Amsterdam [u.a.]
|b Elsevier
|c 2006
300 _ _ |a 520 - 525
336 7 _ |a Journal Article
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336 7 _ |a Output Types/Journal article
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336 7 _ |a Journal Article
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336 7 _ |a ARTICLE
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336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |a Thin Solid Films
|x 0040-6090
|0 5762
|y 2
|v 496
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a A dielectric model comprising band gap transitions and free electron excitations (Drude model) is successfully applied to simulate transmittance spectra of ZnO films doped with 0.5%, 1% and 2% Al. The Drude formula contains a frequency-dependent damping term in order to get a good fit in the visible spectral region. Useful physical parameters obtained from the fit are electron density and mobility within the grains, film thickness, band gap and refractive index. The optically determined film thickness agrees with that obtained with the stylus method within 2%. The optically determined electronic parameters are compared with those obtained by electrical measurements. Contrary to thin In2O3:Sn films, the Drude mobility inside the grains is similar to the direct current Hall mobility indicating more perfect film growth without forming pronounced grain boundaries. Maximum value is 35 cm(2)/V s. The effective electron mass is estimated to be about 0.6 of the free electron mass. The refractive index at 550 run decreases with increasing electron density. (c) 2005 Elsevier B.V. All rights reserved.
536 _ _ |a Erneuerbare Energien
|c P11
|2 G:(DE-HGF)
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588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
|2 WoSType
653 2 0 |2 Author
|a zinc oxide (563)
653 2 0 |2 Author
|a electrical properties (112)
653 2 0 |2 Author
|a optical properties (345)
700 1 _ |a Agashe, C.
|b 1
|u FZJ
|0 P:(DE-Juel1)VDB13388
700 1 _ |a Mergel, D.
|b 2
|0 P:(DE-HGF)0
773 _ _ |a 10.1016/j.tsf.2005.08.282
|g Vol. 496, p. 520 - 525
|p 520 - 525
|q 496<520 - 525
|0 PERI:(DE-600)1482896-0
|t Thin solid films
|v 496
|y 2006
|x 0040-6090
856 7 _ |u http://dx.doi.org/10.1016/j.tsf.2005.08.282
909 C O |o oai:juser.fz-juelich.de:57973
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913 1 _ |k P11
|v Erneuerbare Energien
|l Erneuerbare Energien
|b Energie
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914 1 _ |a Nachtrag
|y 2006
915 _ _ |0 StatID:(DE-HGF)0010
|a JCR/ISI refereed
920 1 _ |k IPV
|l Institut für Photovoltaik
|d 31.12.2006
|g IPV
|0 I:(DE-Juel1)VDB46
|x 1
970 _ _ |a VDB:(DE-Juel1)91129
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980 _ _ |a UNRESTRICTED
981 _ _ |a I:(DE-Juel1)IMD-3-20101013
981 _ _ |a I:(DE-Juel1)IEK-5-20101013


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