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@PHDTHESIS{Dederichs:28496,
author = {Dederichs, F.},
title = {{S}ummenfrequenz-{S}chwingungsspektroskopie an der
{P}latin/{F}lüssigkeit-{G}renzfläche},
volume = {3758},
issn = {0944-2952},
school = {Techn. Hochsch. Aachen},
type = {Dr. (FH)},
address = {Jülich},
publisher = {Forschungszentrum, Zentralbibliothek},
reportid = {PreJuSER-28496, Juel-3758},
series = {Berichte des Forschungszentrums Jülich},
year = {2000},
note = {Record converted from VDB: 12.11.2012; Aachen, Techn.
Hochsch., Diss., 2000},
abstract = {The last years have witnessed a tremendous advance in
understanding electrochemical interfaces. These insights
have been mode possible by the impmvement of existing and
the invention of new experimental techniques, respectively .
One of these methods is optical sumfrequency generation
(SFG), which in this work is applied to the investigation of
molecular vibrations at electrolyte/platinum interfaces . As
a second-order nonlinear optical effect, SFG is due to its
inherent interface sensitivity ideally suited for the
spectroscopy of electrochemical interfaces. In order to lay
the foundations for the experimental applications we start
with a theoretical description of sum-frequency generation
and discuss the experimental setup utilized in this work.
The first experimental chapter deals with the chemisorption
of carbon monoxide (CO) onto (111) and (110) platinum (Pt)
single-crystal faces in a CO-saturated 0 .1 M HC1O4 aqueous
electrolyte . Whereas CO adsorbs on Pt(110) only on terminal
sites as indicated by a single vibrational band around 2075
cmil in our sum-frequency spectra, we observe different
adsorption geometries on Pt(111) . For potentials below 0
.37 V/RHE CO adsorbs on terminal and hollow sites of the
(111) face while for higher potentials up to
electro-oxidation of the carbon monoxide at about 0 .55
V/RHE it occupies terminal and Bridge sites, respectively .
We discuss in detail the influence of the electrochemical
thin layer electrolyte in our spectrochernical cell on the
electro-oxidation of CO. We investigate the adsorption of
cyanide (CN) on Pt(111) surfaces by dissociation of
acetonitrile (CH 3CN) molecules from the vapor phase above
liquids containing acetonitrile, followed by irmnersion of
the sample into the liquid . Using optical sum-frequency
generation and cyclic voltammetry we can identify the
adsorbed Spezies unambiguously as cyanide by the
characteristic potential dependencies of the C-N stretching
vibration frequencies and the voltammetric profile in a (0.1
M HC1O4 + 25 M CH3CN) aqueous electrolyte . In neat
acetonitrile we observe two adsorbed states of CN with
vibrational bands at 1861 uni (hollow site) and 2073 cm-'
(on-top site), distinctly below and above that of the
isolated molecule, demonstrating a covalent CN-platinum bond
. We discuss duster calculations which show that the
weakening and strengthening of the C-N bond at the hollow
and on-top sites is due to a surface-induced depletion of
the Bonding In and antibonding 4o orbitals, respectively. In
the last poft of this work we present a sum-frequency study
of the electrochemical interface forrned by (111), (110) and
(100) platinum faces, respectively, with aqueous
electrolytes containing 0.1 M HCIO4. Despite of strong IR
absorption due to water molecules in the bulk electrolyte,
interfacial water vibrations are observed in our SFG spectra
because their bands are dramatically broadened towards lower
frequencies, containing components which are redshifted as
much as 1000 cri ' . We conclude that these frequency shifts
are caused by the strong, inhomogeneous eiearie field at the
electrochemical interface, which weakens the O- -bonds . A
detailed analysis of our sum-frequency spectra, using an
inhomogeneous broadened model function and taking into
account the linear-optical properties of the
three-layer-system CaF 2 (laser window)/aqueous
electrolyte/Pt electrode, allows us to deduce the potential
dependence of the SFG amplitude of the O-H-vibrations. Since
this amplitude of the water vibrations correlates with the
charge density on the platinum electrode surface, we are
able to estimate the potential of zero charge (PZC) of the
Pt electrodes . For Pt(111) in 0 .1 M HCIO4 we obtain a PZC
value of 0 .86 +20-.0128 V/RHE.},
cin = {IGV},
cid = {I:(DE-Juel1)VDB167},
pnm = {Struktur und Dynamik der Grenzflächen},
pid = {G:(DE-Juel1)FUEK261},
typ = {PUB:(DE-HGF)11 / PUB:(DE-HGF)3},
url = {https://juser.fz-juelich.de/record/28496},
}