001     46694
005     20180210125409.0
024 7 _ |2 WOS
|a WOS:000226205000020
037 _ _ |a PreJuSER-46694
041 _ _ |a eng
082 _ _ |a 540
084 _ _ |2 WoS
|a Chemistry, Multidisciplinary
100 1 _ |a Garcia, S. G.
|b 0
|0 P:(DE-HGF)0
245 _ _ |a In Situ STM Study of Electrocrystallization of Ag on Ag(111)
260 _ _ |a São Paulo
|b SBQ
|c 2004
300 _ _ |a 917
336 7 _ |a Journal Article
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|2 PUB:(DE-HGF)
336 7 _ |a Output Types/Journal article
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336 7 _ |a Journal Article
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|2 EndNote
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |a Journal of the Brazilian Chemical Society
|x 0103-5053
|0 14242
|v 15
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a The electrocrystallization process was studied in the system Ag(111)1Ag(+). SO4= by in situ scanning tunneling microscopy (STM). The results show that Ag deposition occur preferentially at step edges following a layer-by-layer growth mechanism, but polarization and imaging conditions Greatly affect the local kinetics of this process. At STM-tip potentials more positive than the Ag/Ag- equilibrium potential. a local dissolution of the substrate underneath the tip is observed even at low negative substrate overpotentials, at which the overall substrate current density is cathodic. An in sire STM imaging of Ag deposition was possible at sufficiently high negative substrate overpotentials. An estimation of the local deposition current density, however. indicates that the deposition rate underneath the STM-tip is reduced. These results are explained by the presence of an electric field between the STM-tip and the substrate, which affects the potential distribution directly underneath the tip. producing a large shielding of the diffusive flux of Ag+ ions.
536 _ _ |a Kondensierte Materie
|c M02
|2 G:(DE-HGF)
|0 G:(DE-Juel1)FUEK242
|x 0
588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
|2 WoSType
653 2 0 |2 Author
|a Scanning Tunneling Microscopy
653 2 0 |2 Author
|a STM-tip shielding effect
653 2 0 |2 Author
|a silver deposition
653 2 0 |2 Author
|a tip-induced dissolution
700 1 _ |a Mayer, C. E.
|b 1
|0 P:(DE-HGF)0
700 1 _ |a Salinas, D. R.
|b 2
|0 P:(DE-HGF)0
700 1 _ |a Staikov, G.
|b 3
|u FZJ
|0 P:(DE-Juel1)VDB13645
773 _ _ |g Vol. 15, p. 917
|p 917
|q 15<917
|0 PERI:(DE-600)2028738-0
|t Journal of the Brazilian Chemical Society
|v 15
|y 2004
|x 0103-5053
909 C O |o oai:juser.fz-juelich.de:46694
|p VDB
913 1 _ |k M02
|v Kondensierte Materie
|l Kondensierte Materie
|b Materie
|0 G:(DE-Juel1)FUEK242
|x 0
914 1 _ |a Nachtrag
|y 2004
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)73878
980 _ _ |a VDB
980 _ _ |a ConvertedRecord
980 _ _ |a journal
980 _ _ |a I:(DE-Juel1)PGI-3-20110106
980 _ _ |a UNRESTRICTED
981 _ _ |a I:(DE-Juel1)PGI-3-20110106


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