V.-A. Tolhurst et al.
FULL PAPER
H, CH2), 7.46–7.63 (m, 4 H, C6H4N, C6H5), 7.76–7.85 (m, 3 H, tial and double-zeta valence basis set on palladium, platinum, sul-
C6H4N, C6H5), 8.19 (m, 1 H, C6H4N), 9.45 (m, 1 H, C6H4N) ppm. phur, selenium and tellurium together with the Dunning/Huzi-
IR (KBr): ν˜ = 3085 (w), 3052 (w), 2974 (m), 2905 (m), 2854 (w),
1608 (m), 1476 (s), 1439 (s), 1396 (m), 1310 (w), 1273 (w), 1163
naga[31] double zeta basis set on other atoms). Sets of five d-func-
tions were used in the basis sets throughout these calculations. For
(m), 1113 (w), 1063 (w), 1022 (w), 998 (w), 914 (w), 780 (s),m 739 the optimised geometries, harmonic vibrational frequencies were
(s), 704 (w), 684 (m), 611 (w), 484 (m) cm–1. UV/Vis (DMSO)/cm–1: calculated at the B3LYP level. All transition structures possessed
ν˜max (εmol/dm3 mol–1 cm–1) = 33950 (4698). m/z = 432 (M-Cl)+
[
30.84, H 2.37, N 3.00; found C 30.99, H 2.40, N 2.97.
one and only one imaginary frequency, and they were further char-
acterised by following the corresponding normal mode towards
each product and reactant. Single-point energies on B3LYP/
LANL2DZ optimised geometries were calculated at the B3LYP
level with the LANL2augmented:6-311+G(2d,p) basis set,[32] which
incorporates the LANL2 effective core potential and augmented
basis sets on the metals (the large f-polarised valence basis set of
Bauschlicher and coworkers[33] was used for palladium and the
LANL2TZ+(3f) basis set for platinum[34]) together with the 6-
311+G(2d,p) basis set[35–37] on all other atoms (3–11G basis set was
used for tellurium). Energies from these single-point calculations
were combined with the zero-point vibrational energy corrections
from the lower level of theory to yield ΔH0 numbers. Unless other-
wise noted all computed energies quoted in this paper refer to these
final ΔH0 numbers. All calculations were carried out with the
Gaussian 03[38] program.
195Pt(12C12H11N32S)35Cl 432]. C12H11Cl2NPtS (467.28): calcd. C
[PdCl2L3] (3a): Procedure as for [PdCl2L1] using L3 (82 %). 1H
NMR (200 MHz, [D6]DMSO): δ = 4.52, 4.75, (AB spin system, 2
H, CH2), 7.55 (m, 1 H, C6H4N), 7.71 (m, 1 H, C6H4N), 8.08 (m,
1 H, C6H4N), 9.21 (m, 1 H, C6H4N) ppm. IR (KBr): ν˜ = 3076 (m),
3000 (w), 2983 (w), 2958 (s), 2908 (m), 1652 (w), 1606 (s), 1558 (w),
1540 (w), 1480 (s), 1446 (s), 1421 (m), 1381 (m), 1265 (m), 1111
(m), 1060 (w), 1029 (w), 924 (m), 839 (w), 815 (w), 762 (vs), 650
(w), 467 (w), 425 (w) cm–1. UV/Vis (DMSO)/cm–1: ν˜max (εmol
/
dm3 mol–1 cm–1) = 25920 (1100), 32800 (4295). m/z = 328 (M-Cl)
+
[
106Pd(12C7H9N80Se)35Cl 328]. C7H9Cl2NPdSe (363.41): calcd. C
23.13, H 2.50, N 3.86; found C 23.41, H 2.83, N 3.58.
[PtCl2L3] (3b): Procedure as for [PtCl2L1] using L3 (45 %). 1H
NMR (200 MHz, [D6]DMSO): δ = 4.47, 4.70 (AB spin system, 2
H, CH2), 7.53 (m, 1 H, C6H4N), 7.81(m, 1 H, C6H4N), 8.15 (m, 1
H, C6H4N), 9.50 (m, 1 H, C6H4N) ppm. IR (KBr): ν˜ = 3111 (w),
3080 (w), 3005 (w), 2987 (w), 2964 (m), 2910 (m), 1610 (s), 1480
(s), 1447 (s), 1421 (m), 1382 (m), 1270 (m), 1113 (m), 1064 (w), 924
(m), 838 (m), 819 (w), 651 (w)m 560 (w), 468 (w), 433 (w) cm–1.
UV/Vis (DMSO)/cm–1: ν˜max (εmol/dm3 mol–1 cm–1) = 33450 (2071).
CCDC-228118 and CCDC-228119 contain the supplementary
crystallographic data for this paper. These data can be obtained
free of charge from The Cambridge Crystallographic Data Centre
via www.ccdc.cam.ac.uk/data_request/cif.
XYZ Cartesian coordinates for all optimised structures described
in this article are available as Supporting Information (see also the
footnote on the first page of this article).
m/z = 416 (M-Cl)+ 195Pt(12C7H9N80Se)35Cl 416]. C7H9Cl2NPtSe
[
(452.11): calcd. C 18.59, H 2.01, N 3.10; found C 18.56, H 1.99, N
3.01.
Acknowledgments
General Procedure for Heck Reactions: A degassed solution of aryl
halide in dimethylacetamide (5.0 mL, 0.30 molL–1) was added to
the alkene (0.70 mL), NaOAc (2.2 mmol), catalyst, nBu4NCl
(1.1 equiv.) and HCO2Na (1.1 equiv.) in a Schlenk vessel under ar-
gon. The reaction was heated at the appropriate temperature for
3–48 hours. The reaction was then cooled to room temperature,
after which 0.20 mL diethylene glycol monobutyl ether was added.
An aliquot (1.00 mL) was taken from the reaction, diluted with
CH2Cl2, and washed three times with a saturated aqueous solution
of NaCl. The organic layer was dried over MgSO4. The conversion
of aryl halide and the E/Z product ratio of ethyl 3-(4-acetylphenyl)-
3-phenyl-2-propenoate were then determined by GC.
We acknowledge the Australian Research Council for funding this
project. We also thank Johnson-Matthey for the generous loan of
PtCl2 and PdCl2, and Prof. W. Levason and Dr. G. Reid for the
[PdCl2(MeS(CH2)2SMe)] sample.
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scans, monochromatic Mo-Kα radiation, λ = 0.71073 Å, 2θmax
=
75°). Nt(otal) reflections merging to N unique (Rint cited) after “em-
pirical”/multiscan absorption correction (proprietary software), No
with F Ͼ 4σ(F) being considered “observed” and used in the full-
matrix least-squares refinements. (x, y, z, Uiso)H were refined for 2a
only, constrained in 2b. Neutral atom complex scattering factors
were employed within the context of the Xtal 3.7 program sys-
tem.[26] Pertinent results are given above and in the Tables and Fig-
ures, the latter showing the 50 % probability amplitude displace-
ment ellipsoids for the non-hydrogen atoms, hydrogen atoms having
arbitrary radii of 0.1 Å.
Computational Methods: Full geometry optimisations were carried
out with the use of the B3LYP[27,28] density functional level of
theory combined with the LANL2DZ basis set (which incorporates
the Hay and Wadt[29,30] small-core relativistic effective core poten-
1054
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Eur. J. Inorg. Chem. 2005, 1048–1055