COMMUNICATION
coordinates to the Ni in 3 at the two germanethiolato sulfurs,
it coordinates to the Pd in 4 at the three sulfurs including a
µ-sulfide of the Ge2S2 quadrangle, in addition to the two
thiolate sulfurs, to form a highly distorted square planar
geometry at the Pd. These results are understandable because
Ni has a rather small energy difference between its square
planar and tetrahedral geometries and are in agreement with
the common findings that the palladium(II) favors a square-
planar coordination environment, while the coordination
environment in the complexes of nickel(II) is much more
variable.6
When cluster 3 was heated to 110 °C for 12 h, a slow color
change from green to dark brown was observed. Separation of
the crude products by preparative gel permeation chromatog-
raphy (GPC) gave a major fraction at a significantly short
retention time compared with that of 1, indicating the unex-
pected formation of large clusters.7 The recrystallization of this
fraction from CH2Cl2/EtOH afforded the novel Ge4Ni6S12 cluster
[DmpGe(µ-S)3]4Ni6 (5) as brown crystals in 53% yield.8 As
shown in Figure 3, the cluster is composed of six square planar
Ni2+ and four tetrahedral [DmpGeS3]3- units. The six nickels
form an octahedron as shown by the dotted line with the nickels
occupying its vertexes, and the four DmpGeS3 units cap half
of the trigonal faces. The intramolecular Ni–Ni distances ranging
from 3.078(2) to 3.184(2) do not indicate their significant
interactions. The mean values of Ni–S and Ge–S distances are
Figure 1. Molecular structure of 2. All hydrogen atoms are excluded for
clarity.
(5) Crystal data for 2: C74H74Ge2NiP2S4; monoclinic; C2/c (No. 15); a )
30.814(3) Å, b ) 21.9372(16) Å, c ) 30.454(3) Å; ꢀ ) 127.5838(18)°,
V ) 16311(3) Å3; Z ) 8; T ) 193 K; λ ) 0.71073 Å; F(000) )
5632; µ ) 11.363 cm-1; Fcalcd ) 1.105 g cm-3; 91 233 reflections
(2θ < 55.0°), 18 666 unique (Rint ) 0.093); R1 ) 0.0860 (I > 2σ(I)),
wR2 ) 0.2642 (all data); GOF (on F2) ) 1.367. Crystal data for
Figure 2. Molecular structure of 3. All hydrogen atoms and the crystalline
solvent molecules are excluded for clarity.
j
3·1.5toluene: C94.5H92Ge2NiP2S4; triclinic; P1 (No. 2); a ) 14.0364(14)
Å, b ) 18.010(3) Å, c ) 18.085(3) Å; R ) 106.910(6)°, ꢀ )
107.7173(13)°, γ ) 95.117(2)°, V ) 4086.6(9) Å3; Z ) 2; T ) 193
K; λ ) 0.71073 Å; F(000) ) 1690; µ ) 11.459 cm-1; Fcalcd ) 1.318
g cm-3; 47 524 reflections (2θ < 55.0°), 18 477 unique (Rint ) 0.143);
R1 ) 0.0711 (I > 2σ(I)), wR2 ) 0.2050 (all data); GOF (on F2) )
0.959. Crystal data for 5·CH2Cl2: C97H100Cl2Ge4Ni6S12; monoclinic;
P21/n (No. 14); a ) 22.913(7) Å, b ) 16.604(4) Å, c ) 27.451(11)
Å; ꢀ ) 101.493(10)°, V ) 10234(6) Å3; Z ) 4; T ) 193 K; λ )
Table 1. Selected Bond Lengths (Å) and Angles (deg) for 2 and 3
2
3
Ge(1)–S(1)
Ge(1)–S(2)
Ge(2)–S(1)
Ge(2)–S(2)
Ge(1)–S(3)
Ge(2)-S(4)
Ni(1)–S(3)
Ni(1)–S(4)
Ni(1)–P(1)
Ni(1)–P(2)
S(3)· · ·S(4)
2.2424(13)
2.232(2)
2.245(2)
2.2342(13)
2.1808(13)
2.1884(11)
2.2226(15)
2.231(2)
2.2398(19)
2.2483(18)
2.258(2)
2.2559(18)
2.202(2)
0.71073 Å; F(000) ) 4816; µ ) 25.735 cm-1; Fcalcd ) 1.534 g cm-3
;
96 655 reflections (2θ < 55.0°), 23 294 unique (Rint ) 0.123); R1 )
0.1156 (I > 2σ(I)), wR2 ) 0.3044 (all data); GOF (on F2) ) 1.257.
The structure was solved by heavy-atom Patterson methods and
expanded using Fourier techniques. All calculations were performed
with a Rigaku/MSC CrystalStructure program package except for
refinement which was performed using SHELX-97 by full-matrix least
squares against F2. Anisotropic refinement was applied to all non-
hydrogen atoms. All the hydrogen atoms were put at calculated
positions, except for those of the disordered crystalline solvent
molecules, two toluenes for 3 and a dichloromethane for 5.
2.187(2)
2.2614(17)
2.2643(15)
2.340(2)
2.357(2)
4.079(2)
2.172(2)
2.1656(13)
3.633(2)
S(3)-Ni(1)-S(4)
S(3)-Ni(1)-P(1)
S(3)-Ni(1)-P(2)
S(4)-Ni(1)-P(1)
S(4)-Ni(1)-P(2)
P(1)-Ni(1)-P(2)
dihedrala
109.33(6)
128.66(8)
82.89(6)
162.71(9)
164.36(6)
82.86(6)
87.55(6)
140.6
109.75(7)
108.50(7)
103.03(6)
100.95(7)
103.09(8)
143.0
(6) Cotton, F. A.; Wilkinson, G.; Murillo, G. AdVanced Inorganic
Chemistry, 6th ed.; John Wiley & Sons: New York, 1999; pp 840–842..
(7) Preparative GPC was performed on a LC-908 instrument (Japan
Analytical Industry, Co. Ltd) with a series of Jaigel 1H and 2H
columns, using chloroform as the eluent with 3.5 mL min-1. The
fraction containing 5 was observed at 45 min retention time, while 1
has a significantly longer 49 min retention time.
a Dihedral angles between planes Ge(1)-S(1)-S(2) and Ge(2)-S(1)-S(2).
(8) Synthesis of [DmpGe(µ-S)3]4Ni6 (5). A toluene solution of 3 (200
mg, 0.135 mmol) was heated for 12 h at 110 °C. The crude product
was separated by GPC (CHCl3, 3.5 mL/min) to give a fraction of 45
min retention time, which was further crystallized by EtOH/CH2Cl2
to give 5 (27 mg) as a red crystals. The yield calculated on the basis
of nickels is 53%.1H NMR (500 MHz, CDCl3): δ ) 7.47 (t, J ) 7.6
Hz, 4H, p-CH of Dmp), 6.98 (s, 16H, m-CH of Mes), 6.97 (d, J )
7.6 Hz, 8H, m-CH of Dmp), 2.27 (s, 24H, p-CH3 of Mes), 1.83 (s,
48H, o-CH3 of Mes). Elemental analysis calcd (%) for
C96H100Ge4Ni6S12: C, 50.55; H, 4.42; S, 16.87. Found: C, 49.98; H,
4.02; S, 16.90.
anedithiolate property. Indeed, the S(3)-Ni(1)-S(4) bond
angle for 3 becomes considerably larger than that for 2, and
the S(3) · · · S(4) distance of 3 is elongated accordingly by
0.45 Å from that of 2 (Table 1). Of note is the fact that the
structure of 3 is completely different from that of the Ge2PdS4
cluster 4 (Scheme 1) obtained from the analogous reaction
using Pd(PPh3)2Cl2. Whereas the dithiadigermetanedithiolate
1902 Inorganic Chemistry, Vol. 47, No. 6, 2008