Inorganic Chemistry
Article
LcBr2AuPMe2Ph (4). LcBr2 (0.0704 g, 0.11 mmol) and KOtBu
(0.0240 g, 0.22 mmol) were combined in 10 mL of dry THF. The
mixture was purged with argon for 5 min and allowed to stir at room
temperature under argon overnight. Me2PhPAuCl (0.0330 g, 0.11
mmol) was then transferred to the reaction mixture, and the resulting
mixture was purged with argon for 5 min and allowed to stir at room
temperature under argon for 48 h. THF was removed under vacuum,
leaving a lustrous residue. Benzene was added, and the solution was
filtered through Celite. The filtrate was heated to 40 °C, and benzene
was removed under vacuum. Trituration of the residue with pentane
led to the isolation of a lustrous powder. This powder was then
dissolved in benzene, and vapor diffusion of pentane into the benzene
solution led to the isolation of dark red crystals. Yield: 0.0300 g, 28%.
ASSOCIATED CONTENT
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S
* Supporting Information
Absorption and emission of 2, 3, and 4; Kohn−Sham orbital
energy level diagrams of 2−5, and optimized Cartesian
coordinates of 1−5 calculated by density-functional theory as
described in the Experimental Section. This material is available
AUTHOR INFORMATION
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Corresponding Author
Notes
1
31P{1H} (C6D6) δ (ppm), −0.79; H (C6D6) δ (ppm) 8.10−8.13 (m,
The authors declare no competing financial interest.
4H), 7.94−7.96 (m, 4H), 7.03−7.07 (m, 5H), 6.95−7.00 (m, 3H),
6.89−6.92 (m, 2H), 6.83−6.85 (m, 5H), 3.38 (s, 6 h), 0.49 (d, 6H, J =
10.4 Hz). Anal. Calcd. for C42H35AuBr2N3O2P: C, 50.37; H, 3.52; N,
4.20. Found: C, 50.65; H, 3.27; N, 4.01. UV−vis (2-MeTHF): λ (ε)
312 nm (8.6 × 103 M−1 cm−1), 595 nm (5.47 × 104 M−1 cm−1);
Emission (2-MeTHF, ex. 312 nm): 372 nm.
ACKNOWLEDGMENTS
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The authors thank the National Science Foundation (Grant
CHE-1057659 to T.G.G.) for support. The diffractometer at
Case Western Reserve was funded by NSF Grant CHE-
0541766. N.D. thanks the Republic of Turkey for a fellowship.
We thank Dr. T. S. Teets for experimental assistance and
Professor D. G. Nocera (both then at the Massachusetts
Institute of Technology) for access to instrumentation. We
thank also Dr. Matthias Zeller, Youngstown State University,
for assistance with the crystallography.
LdBr2AuPMe2Ph (5). LdBr2 (0.1040 g, 0.11 mmol) and KOtBu
(0.0240 g, 0.22 mmol) were combined in 10 mL of dry THF. The
mixture was purged with argon for 5 min and allowed to stir at room
temperature under argon overnight. Me2PhPAuCl (0.0330 g, 0.11
mmol) was then transferred to the reaction mixture. The resulting
mixture was purged with argon for 5 min and allowed to stir at room
temperature under argon for 48 h. THF was removed under vacuum,
leaving a lustrous residue. Benzene was added, and the solution was
filtered through Celite. The filtrate was heated to 40 °C, and benzene
was removed under vacuum. Trituration of the residue with pentane
led to the isolation of a lustrous powder. This powder was then
dissolved in benzene, and vapor diffusion of pentane into the benzene
solution led to the isolation of a dark greenish powder. Yield: 0.0638 g,
47%. 31P{1H} (C6D6) δ (ppm), −1.81; 1H (C6D6) δ (ppm) 7.68−7.72
(m, 4H), 7.46−7.49 (m, 4H), 7.31−7.34 (m, 4H), 7.11−7.12 (m, 4H),
7.00−7.02 (m, 3H), 6.71−6.76 (m, 2H), 0.42 (d, 6H, J = 10.4 Hz).
Anal. Calcd. for C40H27AuBr6N3P: C, 38.22; H, 2.16; N, 3.34. Found:
C, 38.15; H, 2.06; N, 3.14. UV−vis (2-MeTHF): λ (ε) 315 nm (3.54
× 103 M−1 cm−1), 605 nm (7.24 × 103 M−1 cm−1); Emission (2-
MeTHF, ex. 312 nm): 355 nm, 467 nm.
X-ray Single Crystal Structure Analysis. Single crystal X-ray
data were collected on a Bruker AXS SMART APEX CCD
diffractometer using monochromatic Mo Kα radiation with the ω
scan technique. The unit cells were determined using SMART39 and
SAINT+.40 Data collection for all crystals was conducted at 100 K
(−173.5 °C). All structures were solved by direct methods and refined
by full matrix least-squares against F2 with all reflections using
SHELXTL.41 Refinement of extinction coefficients was found to be
insignificant. All non-hydrogen atoms were refined anisotropically. All
hydrogen atoms were placed in standard calculated positions, and all
hydrogen atoms were refined with an isotropic displacement
parameter 1.2 times that of the adjacent carbon.
Calculations. Spin-restricted density-functional theory calculations
were performed within Gaussian 09 rev. A.02.42 Geometries were
optimized without imposed symmetry. Calculations employed the
exchange and correlation functionals of Perdew, Burke, and
Ernzerhof,43 and the TZVP basis set of Godbelt, Andzelm, and co-
workers for carbon, hydrogen, oxygen, and phosphorus.44 For gold,
the Stuttgart 97 effective core potential and basis set were used;45
scalar relativistic effects are included implicitly. Harmonic frequency
calculations returned all real vibrational frequencies. The calculations,
including geometry optimizations, impose continuum solvation in
THF, using the integral equation formalism of Tomasi’s polarizable
continuum model.46−49 Population analyses were performed with the
AOMIX-CDA software of Gorelsky.50,51
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