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217
10.6 Hz), 119.28 (dd, J(13C–19F) = 5.3, 17.9 Hz), 103.95 (t,
J(13C–19F) = 24.9 Hz) ppm. 19F NMR (CDCl3): d ꢀ110.55 (d, J =
5.3 Hz) ppm. Anal. Calc. for C12H6F4Hg: C, 33.77; H, 1.42. Found:
C, 34.05; H, 1.54%.
and the associated basis set [28], which was contracted as fol-
lows: (8s,7p,6d) ? [6s,5p,3d]. Full D2d symmetry was imposed
during optimization; a harmonic frequency calculation of the
optimized structure confirmed it to be a potential-energy mini-
mum. A single-point calculation was performed on the resulting
optimized geometry. In this calculation, nonmetal atoms were de-
scribed with the TZVP basis set of Godbout and co-workers [29].
The Stuttgart effective core potential and basis set were again
used for mercury. Relativistic effects with the Stuttgart ECP and
its associated basis set are introduced with a potential term
(i.e., a one-electron operator) that replaces the two-electron ex-
change and Coulomb operators resulting from interaction be-
tween core electrons and between core and valence electrons.
In this way relativistic effects, especially scalar effects, are in-
cluded implicitly rather than as four-component, one-electron
functions in the Dirac equation. Methylene chloride solvation ef-
fects were included implicitly with the polarized continuum mod-
el (PCM) of Tomasi and co-workers [30,31]. Percentage
compositions of molecular orbitals, overlap populations, and bond
orders between fragments were calculated using the AOMIX pro-
gram [32,33].
3.1.8. [Hg(2-methyl-5-fluorophenyl)2] (8)
The isolated solid was analytically pure. Yield: 50 mg (58%). 1H
NMR (CDCl3): d 7.28 (dd, C6FH3(CH3), J = 5.2, 8.4 Hz, 2H), 7.09 (dd,
C6FH3(CH3), J = 2.8, 8.4 Hz, 2H), 6.85 (td, C6FH3(CH3), J = 2.8, 8.4 Hz,
2H), 2.53 (s, C6FH3(CH3), 6H) ppm. 13C NMR (CDCl3): d 162.83 (s),
160.37 (s), 139.87 (d, J(13C–19F) = 3.4 Hz), 131.10 (d, J(13C–19F) =
6.7 Hz), 123.09 (d, J(13C–19F) = 18.1 Hz), 114.60 (d, J(13C–19F) =
21.1 Hz), 24.55 (s, C6H3F(CH3)) ppm. 19F NMR (CDCl3):
d
(ꢀ119.08)–(ꢀ119.29) (m) ppm. Anal. Calc. for C14H12F2Hg: C,
40.15; H, 2.89. Found: C, 39.99; H, 2.66%.
3.1.9. [Hg(2-benzothienyl)2] (9)
The isolated solid was analytically pure. Yield: 34 mg (80%). The
product is sparingly soluble only in DMSO, and only 1H NMR solu-
tion data could be obtained. 1H NMR (DMSO-d6): d 7.95 (d,
J = 8.0 Hz, 2H), 7.86 (d, J = 6.8 Hz, 2H), 7.51 (s, 2H), 7.25–7.36 (m,
4H) ppm. Anal. Calc. for C16H10HgS2: C, 41.15; H, 2.16. Found: C,
40.27; H, 1.97%.
Acknowledgements
3.2. Crystal structure determination of compound 6
D.V.P. gratefully acknowledges investors in Creative Chemistry,
LLC and Case Western Reserve University for support. T.G.G. grate-
fully acknowledges the National Science Foundation (Grant CHE-
0749086), the donors of the Petroleum Research Fund adminis-
tered by the American Chemical Society (Grant 42312-G3 to
T.G.G.), and Case Western Reserve University for support. Mr.
James B. Updegraff III is thanked for assistance with crystallo-
graphic work for 6.
3.2.1. Crystal data
Compound 6: C10H8HgN2, M = 356.77, orthorhombic, space
group Ibca, a = 11.0574(17) Å, b = 21.975(4) Å, c = 30.710(5) Å, U =
7462(2) Å3, Z = 32, Dcalc = 2.543 Mg mꢀ3, k (Mo k
a) = 0.71069 Å,
l
= 16.450 mmꢀ1, F(000) = 5184, T = 100(2) K.
3.2.2. Data collection and reduction
A colorless block ca. 0.53 ꢁ 0.31 ꢁ 0.05 mm3 (grown by slow
diffusion of pentane into a saturated 1,2-dichloroethane solution)
was mounted in paratone oil on a mitogen tip. A total of 40290
reflections were collected on a Bruker AXS SMART APEXII CCD dif-
fractometer, h ranging from 1.85–27.23° for data collection. A Lor-
entz-polarization type absorption correction was applied using
AXScale. Merging equivalents gave 4139 independent reflections
(Rint = 0.0678).
Appendix A. Supplementary material
CCDC 702269 contains the supplementary crystallographic data
for compound 6. These data can be obtained free of charge from
article can be found, in the online version, at doi:10.1016/
3.2.3. Structure solution and refinement
References
The unit cell was determined using APEX2 Crystallographic
Suite. The structure of 6 was solved by direct methods and refined
by full matrix least squares against F2 with all reflections using
SHELXTL. Refinement of extinction coefficients was found to be insig-
nificant. All non-hydrogen atoms were refined anisotropically. All
other hydrogen atoms were placed in standard calculated positions
and all hydrogen atoms were refined with an isotropic displace-
ment parameter 1.5 (CH3) or 1.2 (all others) times that of the adja-
cent carbon or nitrogen atom. The refinement proceeds to R1 =
0.0231, wR2 = 0.0823 with a goodness of fit on F2 0.820 for 299 re-
fined parameters and 0 restraints, and R1 = 0.0367, wR2 = 0.1095
for all data with electron density ranging from 1.417 to
ꢀ1.781 e Å3 in the final Fourier synthesis.
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