5356 Organometallics, Vol. 29, No. 21, 2010
Yao et al.
4
and its subsequent coupling with another molecule of 1, DFT
calculations have been performed. The proposed mechanism
involving the reactive intermediates 1a and 1b and part of the
calculated potential energy surface are shown in Scheme 3
and Figure 3, respectively. The isomerization is initiated by a
nucleophilic attack of the methylene subunit in resonance
structure 10 to the Ge(II) center and the concomitant forma-
tion of an excocyclic imine group to give the intermediate 1a.
The barrier for the isomerization step 1 f 1a was calcu-
lated to 29.4 kcal mol-1, thus indicating a slow but yet achie-
vable process at room temperature. 1a is ca. 9.4 kcal mol-1
higher in energy than 1 due to sacrificing one of the stabiliz-
ing N-Ge interactions. However, transient 1a can undergo
an imine-enamine tautomerization by transferring a proton
from C1 to N1 to give 1b; the latter gains extra stabilization
through six π-electron delocalization. Such a proton-transfer
process can be accelerated in the presence of a suitable base.
With NH3, acting as an external model to mimic HN(SiMe3)2,
7.06 (d, JHH = 2.8 Hz, 1 H, R-CH), 6.89 - 7.32 (m, 12 H,
2,6-iPr2C6H3). 13C{1H}NMR (100.61 MHz, D8-THF, 298 K): δ
24.1, 26.0, 26.2, 27.2, 28.3, 28.7, 29.7, 30.4 (iPr, NCMe); 97.3, 110.1
(γ-C); 152.1 (R-C); 124.2 - 153.8 (2,6-iPr2C6H3); 160.7, 170.3
(NCMe). Anal. (%) Calcd for C58H82N4Ge2: C 71.20; H 8.24; N
5.73. Found: C 70.97; H 8.27; N 5.37. EI-MS: m/z (%) 978 (0.5,
[M]þ), 490 (33, [1/2M]þ), 475 (100, [1/2M - Me]þ).
Single-Crystal X-ray Structure Determinations. Crystals were
each mounted on a glass capillary in perfluorinated oil and
measured in a cold N2 flow. The data of compounds 2 and 3 were
collected on an Oxford Diffraction Xcalibur S Sapphire at 150 K
˚
(Mo KR radiation, λ = 0.71073 A). The structures were solved
by direct methods and refined on F2 with the SHELX-979 soft-
ware package. The positions of the H atoms were calculated and
considered isotropically according to a riding model.
˚
˚
2: triclinic, space group P1, a= 10.8593(3) A, b= 13.1638(4) A,
˚
c = 14.4489(3) A, R = 92.576(2)°, β = 101.490(2)°, γ =
102.174(2)°, V = 1970.39(9) A , Z = 2, Fcalc = 1.413 Mg/m3,
3
˚
μ(Mo KR) = 0.858 mm-1, 16 016 collected reflections, 6886
crystallographically independent reflections [Rint = 0.0142],
6064 reflections with I > 2σ(l), θmax = 25°, R(Fo) = 0.0264
the relative energy of TS1a/1b amounts to 28.8 kcal mol-1
,
2
which is slightly lower than that of TS1/1a. The N1 atom of
the NH(aryl) moiety in 1b is sterically less congested than that
of HN(SiMe3)2 and thus easily accessible for a 1,4-addition to
1 to give the bis(germylene) 3.
(I > 2σ(l)), wR(Fo ) = 0.0716 (all data), 506 refined parameters.
˚
3: triclinic, space group P1, a = 11.403(3) A, b = 14.520(2) A,
˚
˚
c = 18.793(3) A, R = 78.926(12)°, β = 82.882(17)°, γ =
78.326(16)°, V = 2978.7(10) A , Z = 2, Fcalc = 1.187 Mg/m3,
3
˚
μ(Mo KR) = 1.050 mm-1, 23 925 collected reflections, 10 182
crystallographically independent reflections [Rint = 0.0489],
5230 reflections with I > 2σ(l), θmax = 25°, R(Fo) = 0.0455
Experimental Section
2
(I > 2σ(l)), wR(Fo ) = 0.0938 (all data), 787 refined parameters.
General Considerations. All experiments were carried out
under dry, oxygen-free dinitrogen using standard Schlenk tech-
niques or in an MBraun inert atmosphere drybox containing an
atmosphere of purified nitrogen. Solvents were dried by standard
methods and freshly distilled prior to use. The starting material
LGe was prepared according to literature procedures.7 1H, 13C,
and 19F NMR spectra were recorded with the Bruker spectro-
meters ARX 200 and AV 400, respectively. EI-MS spectra were
taken on a Finnigan-MAT 955 instrument. Elemental analyses
were performed on a FlashEA 1112 CHNS analyzer.
Computational Details
All calculations were performed at the B3LYP level of
theory10 as implemented in the Gaussian03 program package.11
The geometry of compound 2 was optimized with the basis sets
BSI (def2-TZVP for Ge, N, and the C atoms at the two core rings
C4GeN, C3GeN2,12 and with 6-31G for the other atoms). The
NICS values were calculated by the GIAO method with the
Ahlrichs basis set BSII, with VTZ for all the elements.13 The ring
centers were defined by a nonweighted mean of the atom co-
ordinates. The ring plane is defined as the plane through the ring
center for which the sum of the squares of the distance of that
plane to the positions of the atoms forming the ring is minimal.
The positions of the NICS centers are aligned through the ring
center and are orthogonal to the ring plane. All relevant oordi-
nates can be found in the Supporting Information.
Syntheses. Compound 2. A solution of HN(C6F5)2 (0.29 g,
0.81 mmol) inhexane (10mL) was added toa solutionof1 (0.40 g,
0.81 mmol) in hexane (15 mL) at room temperature. The brown-
red color of the reaction mixture changed to yellow immediately.
After concentration and cooling to -20 °C for 24 h, compound 2
crystallized from the solution as yellow crystals (0.62 g, 0.74
mmol, 91%). Mp: 191 °C (dec). 1H NMR (200.13 MHz, C6D6,
298 K): δ 1.06 (d, 3JHH = 7 Hz, 6 H, CHMe2), 1.12 (d, 3JHH
=
7 Hz, 6 H, CHMe2), 1.13 (d, 3JHH = 7 Hz, 6 H, CHMe2), 1.23 (d,
3JHH = 7 Hz, 6 H, CHMe2), 1.52 (s, 6 H, CMe), 3.03 (sept., 2 H,
3JHH = 7 Hz, CHMe2), 3.37 (sept., 2H, 3JHH = 7 Hz, CHMe2),
5.01 (s, 1 H, γ-CH), 7.02-7.20 (m, br, 6 H, aroma-H). 13C{1H}
NMR (50.61 MHz, C6D6, 298 K): δ 24.4, 24.7, 24.8, 25.7, 28.3,
29.3 (iPr, NCMe), 101.7 (γ-C), 125.0-146.2 (2,6-iPr2C6H3,
C6F5), 167.8 (NCMe). 19F{1H} NMR (188.31 MHz, C6D6, 298
K): δ -146 (br), -149 (br), -165.5 (br). Anal. (%) calcd for
C41H41N3GeF10: C 58.74; H 4.93; N 5.01. Found: C 59.31; H
5.05; N 4.96. EI-MS: m/z (%) 491 (15, [M - N(C6F5)2]þ), 475(73,
[M - N(C6F5)2 - Me]þ), 349 (100, [N(C6F5)2]þ).
To study the isomerization 1 f 1a f 1b, the two-layer ONIOM-
(B3LYP/BSIII: B3LYP/3-21G) approach was employed.14 As
shown in Figure 3, the higher layer consists of the core ring and
was calculated with basis sets BSIII (6-311Gþ(d,p) for N and
6-311Gþ(d,p) for other elements). The lower layer consists of the
(9) Sheldrick, G. M. SHELX-97, Program for Crystal Structure
€
€
Determination; Universitat Gottingen: Germany, 1997.
(10) (a) Lee, C.; Yang, W.; Parr, R. G Phys. Rev. B: Condens. Matter
1988, 37, 785. (b) Becke, A. D. J. Chem. Phys. 1993, 98, 5648.
(11) Frisch, M. J.; et al. et al. Gaussian, Inc.: Wallingford, CT, 2004.
(12) Weigend, F.; Ahlrichs, R. Phys. Chem. Chem. Phys. 2005, 7,
3297.
(13) Schafer, A.; Horn, H.; Ahlrichs, R. J. Chem. Phys. 1992, 97,
2571.
Compound 3. To a solution of 1 (0.47 g, 0.96 mmol) in hexane
(20 mL) was added HN(SiMe3)2 (12 mol %) at room temperature.
During the course of 3 weeks yellow crystals of compound 3 were
1
formed (0.23 g, 0.23 mmol, 48%). Mp: 181 °C (dec). H NMR
(14) (a) Maseras, F.; Morokuma, K. J. Comput. Chem. 1995, 16, 1170.
(b) Humbel, S.; Sieber, S.; Morokuma, K. J. Chem. Phys. 1996, 105, 1959.
(c) Matsubara, T.; Sieber, S.; Morokuma, K. Int. J. Quantum Chem. 1996,
60, 1101. (d) Svensson, M.; Humbel, S.; Froese, A. D. J.; Matsubara, T.;
Sieber, S.; Morokuma, K. J. Phys. Chem. 1996, 100, 19357. (e) Svensson,
M.; Humbel, S.; Morokuma, K. J. Chem. Phys. 1996, 105, 3654. (f)
Dapprich, S.; Komꢀaromi, I.; Byun, S.; Morokuma, K.; Frisch, M. T. THEO-
CHEM 1999, 461, 1. (g) Vreven, T.; Morokuma, K. J. Comput. Chem.
3
(200.13 MHz, D8-THF, 298 K): δ 0.10 (d, JHH = 7 Hz, 6 H,
CHMe2), 0.85 (d, 3JHH = 7 Hz, 6 H, CHMe2), 1.08 (d, 3JHH
=
7 Hz, 6 H, CHMe2), 1.10 (d, 3JHH = 7 Hz, 6 H, CHMe2), 1.18 (d,
3JHH = 7 Hz, 6 H, CHMe2), 1.20 (d, 3JHH = 7 Hz, 6 H, CHMe2),
1.25 (d, 3JHH = 7 Hz, 6 H, CHMe2), 1.31 (d, 3JHH = 7 Hz, 6 H,
CHMe2),1.75(s,6H,CMe),2.18(s,3H,CMe),2.53(sept.,3JHH
=
7 Hz, 2 H, CHMe2), 2.30 (sept., 3JHH = 7 Hz, 2 H, CHMe2), 3.39
(sept., 3JHH = 7 Hz, 2 H, CHMe2), 3.59 (sept., 3JHH = 7 Hz, 2 H,
CHMe2), 5.27 (s, 1 H, γ-CH), 6.69 (d, 4JHH = 2.8 Hz, 1 H, γ-CH),
ꢀ
2000, 21, 1419. (h) Vreven, T.; Byun, S.; Komaromi, I.; Dapprich, S.;
Montgomery, J. A., Jr.; Morokuma, K.; Frisch, M. J. J. Chem. Theory
Comput. 2006, 2, 815.