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arylalumylene complexes were obtained in moderate yields
(1a: 72%, 1b: 21%). The complexes 1a and 1b are stable up
to 79 and 1108C, respectively, in the solid state, but they
slowly decompose in solution, even at ꢀ358C, to give
complicated mixtures containing [Pt(PCy3)2] and PCy3.
In the 31P NMR spectra, 1a and 1b exhibit singlets
important.[6d,16] The calculated NBO corresponding to the
ꢀ
Al Pt bond is predominantly formed from the overlap of the
3s(Al) and 6s(Pt) orbitals [s(Al-Pt) = 0.87(3s3p0.03)Al +
0.50(6s6p0.036d0.02)Pt]. Meanwhile, the Pt!Al p-back dona-
tion interactions were identified as donor/acceptor interac-
tions, and the stabilization energies from the two 5d(Pt)!
3p(Al) p-back donations were estimated to be 19.86 and
4.54 kcalmolꢀ1 by using a second-order perturbation theory
accompanied by 195Pt satellites at d = 69.9 ppm (1JPPt
=
4015 Hz) and d = 69.8 ppm (1JPPt = 4033 Hz), respectively,
ꢀ
which are downfield shifted with respect to those of [Pt-
(PCy3)2] (d = 62.3 ppm, JPPt = 4160 Hz) and the structurally
analysis. The nature of the Al Pt bond in 1a was further
1
investigated in terms of the energy decomposition analy-
sis,[17,18] thus showing that the Al-Pt bonding interaction is
mainly electrostatic. The electrostatic interaction contributes
74.0% of the total attractive interactions between the BbpAl
and [Pt(PCy3)2] moieties. The breakdown of the Al-Pt orbital-
interaction energy into s and p components indicates that the
Pt!Al p-back donation significantly contributes to the
covalent bonding (s: 55.8%, p: 44.2%).
related carbonyl complex [(Cy3P)2Pt(CO)] (d = 63.7 ppm,
1JPPt = 4101 Hz).[12] Definite signals could not be observed in
the 27Al and 195Pt NMR spectra of 1a and 1b, probably
because of the signal broadening caused by the high quadru-
pole moment of the 27Al nuclei.
Molecular structures of 1a and 1b were determined by X-
ray crystallographic analyses, thereby showing that the
aluminum atoms are definitely two-coordinate and are
bound to the platinum atoms in a terminal fashion with C1-
Al1-Pt1 angles of 179.2(2) (1a) and 173.96(14)8 (1b;
Figure 2). The platinum centers adopt distorted trigonal-
In summary, the first Lewis-base-free terminal arylalu-
mylene complexes were obtained by two different routes: the
treatment of a dialumene–benzene adduct (2) with [Pt-
(PCy3)2] and the reduction of the 1,2-dibromodialumanes 3
ꢀ
in the presence of [Pt(PCy3)2]. The Al Pt bonds in the
arylalumylene complexes were shortened compared to the
ꢀ
previously reported Al Pt distances, thus indicating the
stronger bonding interactions between the alumylene and
platinum moieties. The DFT calculations suggested that the
ꢀ
Al Pt bonds in the arylalumylene complexes possess signifi-
cantly high electrostatic character and that the contribution of
the Pt!Al p-back donation to the covalent interactions is
comparable to that of the Al!Pt s-donation.
Figure 2. Molecular structures of a) 1a and b) 1b. Thermal ellipsoids
are drawn at the 50% probability level. Hydrogen atoms are omitted,
and the Bbp, Tbb, and Cy groups are shown in wireframe format for
clarity. Three Cy and two Me groups in 1a were disordered over two
positions (see the Supporting Information for details). Selected bond
lengths [ꢀ] and angles [8]: 1a: Al1–Pt1 2.2857(18), C1–Al1 2.001(6),
Pt1–P1 2.2828(17), Pt1–P2 2.2903(16); C1-Al1-Pt1 179.2(2), Al1-Pt1-P1
114.86(6), Al1-Pt1-P2 117.85(6), P1-Pt1-P2 127.29(6). 1b: Al1–Pt1
2.2829(13), C1–Al1 1.986(4), Pt1–P1 2.3071(9), Pt1–P2 2.2673(10); C1-
Al1-Pt1 173.96(14), Al1-Pt1-P1 119.14(4), Al1-Pt1-P2 109.20(4), P1-Pt1-
P2 131.56(4).
Experimental Section
All the manipulations were performed under a dry argon atmosphere
by using the Schlenk techniques and glove boxes. Solvents were
purified by the Ultimate Solvent System, Glass Contour Company[19]
(n-hexane) or by the bulb-to-bulb distillation from a potassium mirror
(C6D6 and mesitylene). [Pt(PCy3)2] was prepared according to
a literature.[20]
Reaction of 2 with [Pt(PCy3)2]: A solution of 2 (13.4 mg,
0.0124 mmol) and [Pt(PCy3)2] (17.4 mg, 0.0230 mmol) in mesitylene
(2 mL) was stirred at room temperature for 2.5 h and then at 508C for
2 h, thus affording a mixture containing 1a and [Pt(PCy3)2] in a ratio
of ca. 1.0:1.5. Small amounts of pure 1a (1.0 mg, 0.00085 mmol, 3%)
were obtained by fractional crystallization from n-hexane at ꢀ358C.
Reduction of 3a in the presence of [Pt(PCy3)2]: To a mesitylene
(5 mL) solution of 3a (13.2 mg, 0.013 mmol) and [Pt(PCy3)2]
(19.0 mg, 0.025 mmol) was added KC8 (3.8 mg, 0.028 mmol). The
mixture was stirred at room temperature for 4.5 h. After removal of
the solvents, the residue was extracted with n-hexane and filtered.
The filtrate was concentrated and stored at ꢀ358C to give 1a as dark
ꢀ
planar geometries. The Pt1 Al1 bonds of the arylalumylene
complexes [1a: 2.2857(18) ꢀ, 1b: 2.2829(13) ꢀ] are slightly
ꢀ
shortened compared to the shortest Pt Al distance previously
reported [2.327(2) ꢀ],[6d] most likely reflecting the decreased
coordination number of platinum as well as the difference in
the aluminum-bound substituents.[13]
To gain further information on the bonding situation in 1a
and 1b, density functional theory (DFT) calculations at the
M062X[14]/SDD[Pt]:6-311G(2df)[Al,P]:6-31G(d)[Si,C,H]
level of theory were performed on a real molecule of 1a. The
comparison of the optimized and experimental bond lengths
and angles of 1a shows that the DFT-optimized structure is
well-matched to that found in the single crystals. The natural
bond orbital (NBO) analysis[15] on the optimized geometry of
1a showed that the Al-Pt bond has a small Wiberg bond index
(0.59), thus indicating that the Al-Pt bond is highly ionic and
that the contribution of the covalent interaction is less
1
red crystals (22.2 mg, 0.019 mmol, 72%). m.p. 798C (dec.); H NMR
(600 MHz, C6D6): d = 0.29 (s, 36H, Si(CH3)3), 1.22–1.43 (m, 24H, Cy),
1.65–1.73 (m, 18H, Cy), 1.90–1.92 (m, 12H, Cy), 2.20–2.22 (m, 12H,
Cy), 2.75 (s, 2H, CH(SiMe3)2), 6.78 (d, 3J = 7.7 Hz, 2H, m-ArH),
7.08 ppm (t, 3J = 7.7 Hz, 1H, p-ArH); 13C{1H} NMR (151 MHz,
C6D6): d = 1.28 (s, SiMe3), 27.1 (s, C4(Cy)), 28.3 (virtual triplet, JCP
=
4.5 Hz, C2,6(Cy),), 31.2 (s, CH(SiMe3)2), 31.3 (s, 4JCPt = 24.1 Hz,
C3,5(Cy)), 41.3 (virtual triplet, JCP = 9.1 Hz, JCPt = 36.2 Hz, C1(Cy)),
2
123.9 (s, 4JCPt = 22.7 Hz, m-C(Ar)), 129.22 (s, p-C(Ar)), 149.4 (s, o-
C(Ar)), 160.0 ppm (t, 3JCP = 25.7 Hz, ipso-C(Ar)); 31P NMR
(120 MHz, C6D6): d = 69.9 ppm (s, 1JPPt = 4015 Hz); UV/vis
3882
ꢀ 2014 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2014, 53, 3881 –3884