A R T I C L E S
Rybtchinski et al.
16.6 Hz, 2JPH ) 9.8 Hz, 1H, Ar-CH2-P, left part of AB system), 3.06
(dd, JPH ) 9.6 Hz, 1H, Ar-CH2-P, right part of AB system), 1.37
set-relativistic effective core potential (RECP) combination35 on the
transition metals. The SDB-cc-pVDZ basis set combines the Dunning
cc-pVDZ basis set36 on the main group elements with the Stuttgart-
Dresden basis set-RECP combination35 on the transition metals, with
an f-type polarization exponent taken as the geometric average of the
two f-exponents given in the Appendix to ref 37.
Geometry optimizations for minima were carried out using the
standard Schlegel algorithm38 in redundant internal coordinates until
in the neighborhood of the solution and then continued using analytical
second derivatives.39 Optimizations for transition states were carried
out by means of the QST3 approach,40 with an initial guess for the
transition state being generated from manual manipulation of the
geometry using MOLDEN.41 In cases where this approach failed to
converge, we used analytical second derivatives at every step.
Zero-point and RRHO (rigid rotor-harmonic oscillator) thermal
corrections (to obtain ∆S, ∆H, and ∆G values) were obtained from
the unscaled computed frequencies.
Where necessary, the Grid ) UltraFine combination, i.e., a pruned
(99 590) grid in the integration and gradient steps and a pruned (50 194)
grid in the CPKS (coupled perturbed Kohn-Sham) steps, was used as
recommended in ref 42.
Zero-point and RRHO (rigid rotor-harmonic oscillator) thermal
corrections were obtained from the unscaled computed frequencies.
Where necessary to resolve ambiguities about the nature of a
transition state, intrinsic reaction coordinate (IRC43) calculations were
carried out. In some cases where IRC calculation failed for technical
reason, displacements were made along the normal coordinate for the
imaginary frequencies and optimizations started from there. While this
pseudo-IRC procedure is less unambiguous than IRC, it at least offers
some form of corroboration.
2
3
3
(d, JPH ) 13.7 Hz, 9H, P-C(CH3)3), 1.22 (d, JPH ) 13.3 Hz, 9H,
P-C(CH3)3), -24.07 (br s, 1H, Rh-H). 13C{1H} NMR (THF-d8):
150.23 (m, Cipso-Rh, Ar), 135.28 (s, Ar), 125.10 (s, Ar), 123.95 (s,
1
Ar), 123.71 (s, Ar), 123.55 (s, Ar), 36.29 (d, JPC ) 16.9 Hz,
P-C(CH3)3), 35.42 (d, 1JPC ) 26.9 Hz, P-C(CH3)3), 33.98 (br d, 1JPC
) 33.8 Hz, Ar-CH2-P), 30.14 (m, P-C(CH3)3), 29.44 (br s,
P-C(CH3)3).
1
Complex 4c. 31P{1H} NMR (methanol-d4): 109.82 (br d, JRhP
)
1
175.8 Hz). H NMR (methanol-d4): 7.43 (br d, JHH ) 7.3 Hz, 1H,
Ar-H), 6.98 (br d, JHH ) 7.2 Hz, 1H, Ar-H), 6.82 (m, 2H, Ar-H), 3.25
(ddd, 2JHH ) 16.7 Hz, 2JPH ) 10.2 Hz, 3JRhH ) 2.2 Hz, 1H, Ar-CH2-
2
P, left part of AB system), 3.06 (dd, JPH ) 9.9 Hz, 1H, Ar-CH2-P,
3
right part of AB system), 1.33 (d, JPH ) 13.6 Hz, 9H, P-C(CH3)3),
3
1
1.21 (d, JPH ) 13.0 Hz, 9H, P-C(CH3)3), -22.66 (dd, JRhH ) 33.2
Hz, 2JPH ) 26.5 Hz, 1H, Rh-H). 13C{1H} NMR (methanol-d4): 150.40
(br d, 1JRhC ) 36.8 Hz, Cipso-Rh), 150.25 (m, Ar), 135.41 (s, Ar), 135.16
1
(s, Ar), 125.35 (m, Ar), 124.02 (m, Ar), 36.23 (d, JPC ) 17.0 Hz,
P-C(CH3)3), 35.48 (d, 1JPC ) 27.6 Hz, P-C(CH3)3), 34.28 (br. d, 1JPC
) 34.1 Hz, Ar-CH2-P), 30.09 (m, P-C(CH3)3), 29.33 (br s,
P-C(CH3)3).
ES MS positive mode (m/e): calcd for C16H29OPRh (one MeOH
molecule remains coordinated) MH+, 371.28; found MH+, 371.12. ES
MS negative mode (m/e): calcd for BF4, 86.80; found, 86.91.
Anal. Calcd for C16H29OPRh (assuming one MeOH molecule remains
coordinated): C, 41.95; H, 6.38. Found: 41.93; 6.44.
Deuteration Experiments. In a typical experiment, complex 4 (15
mg, 0.040 mmol) was dissolved in a solvent of choice (CD3OD or
acetone/D2O (5:1 v/v) mixture). Styrene (about 70 equiv) was added
to the solution of 4, and the resulting mixture was placed in the screw-
cap NMR tube and was heated for 24 h at 65 °C. Toluene-d8 (20 µL)
was added to the reaction mixture as a standard, and the integrals of
the signals of vinylic deuterons in 2D NMR were compared to those of
tolune-d8. In all the cases exclusive vinylic deuteration was observed.
Formation of styrene-d3 was confirmed by GC-MS.
For interpretative purposes, atomic partial charges and Wiberg bond
indices44 were obtained by means of a natural population analysis
(NPA)45 at the mPW1k/SDD level.
The energetics for our final reaction profile were validated by single-
point energy calculations, using the mPW1k/SDD reference geometries,
at the higher level of theory mPW1k/SDB-cc-pVDZ.
Acknowledgment. This work was supported by the Israel
Science Foundation (Grant No 83/00), the MINERVA founda-
tion, Munich, Germany, the Tashtiyot program of the Ministry
of Science (Israel), the Israel Inter-University Computing Center,
and the Helen and Martin Kimmel Center for Molecular Design.
We thank Dr. Leonid Konstantinovsky for the help with NMR
measurements. D.M. holds the Israel Matz Professorial Chair
in Organic Chemistry. J.M.L.M. is a member of the Lise
Meitner-Minerva Center for Computational Quantum Chemistry.
Computational Methods
All calculations were carried out using the Gaussian 98 program
revision A.1132 running on Compaq ES40 and XP1000 workstations
as well as on a mini-farm of Pentium IV Xeon 1.7/2.0 GHz PC’s
running Red Hat Linux 7.2 in our group, on an experimental Linux
PC Farm at the Faculty of Physics, and on the (Israel) Inter-University
Computing Center (IUCC) SGI Origin 2000.
The mPW1k (modified Perdew-Wang 1-parameter for kinetics)
exchange-correlation functional of Truhlar and co-workers33 was
employed in conjunction with the SDD and SDB-cc-pVDZ basis sets
(see below). The mPW1k functional was very recently shown28b,33,34
to yield more reliable reaction barrier heights than other exchange-
correlation functionals.
Supporting Information Available: XYZ coordinates of all
computed structures and SST spectrum of complex 4b (PDF).
This material is available free of charge via the Internet at
The SDD basis set is the combination of the Huzinage-Dunning
double-ú basis set on lighter elements with the Stuttgart-Dresden basis
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