EXAFS Studies in the Mizoroki–Heck Reaction
FULL PAPER
in fluorescence mode by a solid-state 13-element germanium detector
tuned to the PdKa fluorescence peak.The solution sample (ca.4 mL) was
injected into a custom-built XAS cell (see Supporting Information) con-
structed from stainless steel.In addition, at the front of the cell, alumini-
um windows (20 mm thick) were mounted to permit the entrance of X-
rays into the sample and allow fluorescence to be collected.This cell was
mounted at about 458 to the direction of the incoming beam with the de-
tector at 908 in the horizontal plane to maximise the fluorescence/scatter
ratio.In addition, the stainless steel cell was mounted to an FC 64 flange
to allow the cell to be positioned inside a six-way cross to provide a
vacuum sleeve and thereby prevent any problems caused by formation of
ice crystals on the cell windows.Typically, six scans were collected at the
Pd K-edge and summed prior to curve fitting.Background-subtracted
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EXAFS data were obtained by using the programme PAXAS. Spheri-
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Organo-
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cal wave curve fitting analysis was executed in EXCURV98, using ab
initio phase shifts and backscattering amplitudes calculated by using
Von-Barth ground state potentials and Hedin–Lundqvist exchange poten-
tials.Fourier transforms of the EXAFS spectra were used to obtain an
approximate radial distribution function around the central transition
metal atom; the peaks of the FT can be related to shells of surrounding
backscattering atoms, which are characterised by atom type, number of
atoms in the shell, the absorber–scatterer distance and the Debye–Waller
factor, a measure of both the thermal motion between the absorber and
scatterer and the static disorder of the absorber–scatterer distances.The
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k -weighted parameters are presented in Table 1 in the Supporting Infor-
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considered to be 1.4 and 1.6% respectively. Precision in 1st shell coor-
dination numbers is estimated to be about 5–10% and between 10 and
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E
3
2
[
0% for non-bonded shells.The R factor is defined as(s
A
H
R
U
G
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E
3
T
E
c ]k dk)100% where c and c are the theoretical and experimental
EXAFS and k is the photoelectron wave vector.
[
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We thank Johnson-Matthey Catalysts for support of part of this project
and generous loan of Pd salts, the EPSRC for support (to N.T. and
A.A.D.), the staff of the ESRF for their assistance and the Directors for
access to the ESRF.
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Received: September 5, 2006
Revised: November 24, 2006
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Published online: February 16, 2007
Chem. Eur. J. 2007, 13, 3652 – 3659
ꢀ 2007 Wiley-VCH Verlag GmbH & Co.KGaA, Weinheim
3659