2458 Organometallics, Vol. 29, No. 11, 2010
Hopmann et al.
3154 (13 157) were independent with a Rint = 0.0342 (0.0408).
Analysis of the data showed no significant decay during the data
collection. Data were corrected for absorption effects using the
multiscan technique SADABS65 with minimum and maximum
transmission coefficients of 0.7293 and 0.8550 (0.8488 and
0.9641), respectively.
rhodium, where we used LANL2DZ (corresponding to the Los
Alamos Effective Core Potential plus DZ74). Additional calculations
employing an added f-polarization function on rhodium (coefficient
= 0.4 (LANL2DZþf040) or 1.35 (LANL2DZþf135))75,76 yielded
virtually identical geometries and similar energies (see Tables S6 and
S7, Supporting Information).
Structures were solved by the direct methods package
SIR9766 and refined using the WinGX software package67
incorporating SHELXL.68 The final anisotropic full-matrix
least-squares refinement on F2 with 164 (651) variables con-
verged at R1 = 0.0219 (0.0436) for the observed data and wR2
= 0.0543 (0.1055) for all data. The GOF was 1.105 (1.060). The
Frequency calculations were performed on all optimized
structures at the same level of theory as geometry optimizations.
Minima exhibited only positive frequencies, while all transition
states exhibited one negative frequency. Thermochemical data
and temperature corrections were computed at 298.15 K for all
optimized geometries. Additional thermochemistry calculations
at 342 K were performed with the freqchk functionality imple-
mented in Gaussian 03. Single-point calculations in CH3CN
solvent (dielectric constant = 36.64) and CHCl3 (dielectric
constant = 4.9) were performed with the solvent model
IEFPCM.
largest peak on the final difference electron density synthesis was
-3
0.53 e A at 0.88 A from Rh and the deepest hole -0.60 e A-3 at
˚
˚
˚
-3
˚
0.91 A from Rh (1.88 e A at 0.86 A from Rh2 and the deepest
hole -0.79 e A at 0.60 A from Rh2). The aromatic, methylene,
and methyl H atoms were placed in geometrically idealized
˚
˚
-3
˚
˚
˚
positions (C-H = 0.93-0.98 A) and constrained to ride on
their parent atoms with Uiso(H) = 1.2Ueq(C) for aromatic and
methylene and Uiso(H) = 1.5Ueq(C) for methyl. The methyl H’s
were located from a Fourier difference map and refined as a rigid
rotor. Non-hydrogen atoms were refined with anisotropic dis-
placement parameters. Atomic scattering factors were taken
from the International Tables for Crystallography Volume C.69
The molecular plot was drawn using the DIAMOND program70
with a 30% thermal envelope probability for non-hydrogen
atoms. Hydrogen atoms were drawn as arbitrarily sized spheres
Acknowledgment. This work was supported by the
Research Council of Norway and the National Research
Foundation of the Republic of South Africa (Grant
Unique Number 65507).
Supporting Information Available: Crystallographic data in
CIF format, optimized Cartesian coordinates, computed thermo-
chemical data for selected systems, and additional figures. This
acs.org.
˚
with a radius of 0.135 A.
The refinement of the two [Rh(PhCOCHCOCH2CH3)(CO)-
(PPh3)] isomers showed large thermal vibrations in the CH2CH3
chain. This was treated by disordered refinement techniques to
obtain more satisfactory refinement parameters. The refinement
was kept stable with additional geometric and anisotropic
restraints. Site occupancies for the terminal carbons in the ethyl
groups of both isomers were left to refine freely but restricted to
add up to one for each methyl, resulting in 0.737:0.263 for C1A
and C1B and 0.664:0.336 for C31A and C31B (Figure 1).
Computational Details. All calculations were performed with
the hybrid DFT functional B3LYP71,72 as implemented in the
Gaussian 03 program package.73 Geometries were optimized in the
gas phase with the triple-ζbasis set 6-311G(d,p) on all atoms except
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Robb, M. A.; Cheeseman, J. R.; Montgomery, J. A., Jr.; Vreven, T.;
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