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001     40341
005     20180210143011.0
024 7 _ |2 DOI
|a 10.1016/S0039-6028(01)01106-2
024 7 _ |2 WOS
|a WOS:000170230200008
037 _ _ |a PreJuSER-40341
041 _ _ |a eng
082 _ _ |a 540
084 _ _ |2 WoS
|a Chemistry, Physical
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |a Pflitsch, C.
|0 P:(DE-Juel1)VDB5560
|b 0
|u FZJ
245 _ _ |a Preparation of a well ordered iron oxide on Cu(110)
260 _ _ |a Amsterdam
|b Elsevier
|c 2001
300 _ _ |a 32
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
|2 PUB:(DE-HGF)
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|0 0
|2 EndNote
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |a Surface Science
|x 0039-6028
|0 5673
|v 488
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a We have grown an ultra-thin film of iron oxide by oxidising a smooth epitaxial 5 ML Fe film which was deposited on Cu(110). In order to prevent roughening of the Fe film, the oxidation of the iron took place at 130 K. At low oxygen exposures, <2 x 10(-6) mbars, a surface oxide forms. After completion of the surface oxide layer a disordered Fe2O3 film grows. Upon annealing, ordering of the oxide film is observed at temperatures above 400 K. A Fe2O3 film With a very well ordered surface could be produced by heating the disordered oxide film. The ordered oxide surface shows a (21 x 6) reconstruction, which is interpreted as a coincidence lattice of the Cu(110) substrate and it Fe2O3(111) lattice which is slightly distorted due to a misfit with the substrate (0.7-2%) and to a misalignment between the major crystallographic axes of the lattices. When the oxide film is slowly heated, decomposition of the oxide takes place in two stages: Between 550 and 700 K, the Fe2O3 film decomposes due to a reaction of this oxide with a buried layer of Fe or FeO. Between 700 and 800 K a further decomposition of the Fe2O3 is found, but now accompanied by desorption of oxygen and solution of Fe in the Cu substrate. The amount of oxygen and iron on the surface keeps on decreasing after the almost complete decomposition of Fe2O3 (at 800 K) until a new phase is obtained which is stable between 950 and 1100 K, This high temperature phase (T > 950 K) shows a (n x 8) reconstruction with n = 17-19. This reconstruction is interpreted as the result of a coincidence lattice of the Cu(110) substrate with a distorted FeO(111) lattice. (C) 2001 Elsevier Science B.V. All rights reserved.
536 _ _ |a Grenzflächenaspekte der Informationstechnik
|c 29.35.0
|2 G:(DE-HGF)
|0 G:(DE-Juel1)FUEK61
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588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
|2 WoSType
653 2 0 |2 Author
|a atom-solid scattering and diffraction - elastic
653 2 0 |2 Author
|a auger electron spectroscopy
653 2 0 |2 Author
|a copper
653 2 0 |2 Author
|a iron
653 2 0 |2 Author
|a iron oxide
653 2 0 |2 Author
|a epitaxy
653 2 0 |2 Author
|a growth
653 2 0 |2 Author
|a surface structure, morphology, roughness, and topography
700 1 _ |a David, R.
|0 P:(DE-Juel1)VDB5790
|b 1
|u FZJ
700 1 _ |a Verheij, L. K.
|0 P:(DE-Juel1)VDB5574
|b 2
|u FZJ
700 1 _ |a Franchy, R.
|0 P:(DE-Juel1)VDB5400
|b 3
|u FZJ
773 _ _ |a 10.1016/S0039-6028(01)01106-2
|g Vol. 488, p. 32
|p 32
|q 488<32
|0 PERI:(DE-600)1479030-0
|t Surface science
|v 488
|y 2001
|x 0039-6028
909 C O |o oai:juser.fz-juelich.de:40341
|p VDB
913 1 _ |k 29.35.0
|v Grenzflächenaspekte der Informationstechnik
|l Grundlagenforschung zur Informationstechnik
|b Informationstechnik
|0 G:(DE-Juel1)FUEK61
|x 0
914 1 _ |y 2001
915 _ _ |0 StatID:(DE-HGF)0010
|a JCR/ISI refereed
920 1 _ |k ISG-3
|l Institut für Grenzflächen und Vakuumtechnologien
|d 31.12.2006
|g ISG
|0 I:(DE-Juel1)VDB43
|x 0
970 _ _ |a VDB:(DE-Juel1)5385
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980 _ _ |a journal
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980 _ _ |a UNRESTRICTED
981 _ _ |a I:(DE-Juel1)PGI-3-20110106

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