Angewandte
Chemie
Figure 1. Crystal structure of [(DipNPPh2)2Li4nBu2] (2). The thermal
ellipsoids are shown at 30% probability. Hydrogen atoms have been
omitted for clarity. Only the main components of the disordered n-
butyl groups are shown. Selected bond lengths [ꢀ] and angles [8]: P1–
N1 1.6786(13), P2–N2 1.6785(13), Li1–N1 2.034(3), Li1–P2 2.560(3),
Li2–N2 2.072(3), Li2–P1 2.591(3), Li3–N1 2.023(2), Li3···P1 2.962(3),
Li4–N2 2.018(3), Li4–P2 2.884(3), Li2–C49 2.256(3), Li3–C49 2.218(3),
Li4–C49 2.202(3), Li1–C53 2.270(3), Li3–C53 2.217(3), Li4–C53
2.245(3), Li1···Li2 3.218(4), Li1···Li3 2.407(4), Li1···Li4 2.856(4); N1-P1-
Li2 94.89(7), P1-N1-Li1 112.26(10), P1-N1-Li3 105.92(10), Li3···Li1···Li4
57.04(10), Li3···Li1···Li2 58.67(10), Li4···Li1···Li2 46.57(8), Li4···Li2···Li3
57.07(10), Li4···Li2···Li1 58.84(10), Li3···Li2···Li1 46.29(8), Li1···Li3···Li4
70.40(12), Li1···Li3···Li2 75.04(11), Li4···Li3···Li2 53.11(10),
Figure 2. Crystal structure of [{(DipNPPh2)Li}4(LiH)4]·C6H6, (3·C6H6).
The thermal ellipsoids are shown at 30% probability. The solvent
molecule and hydrogen atoms except hydride ligands have been
omitted for clarity. Selected bond lengths [ꢀ] and angles [8]: P1–N1
1.666(2), P2–N2 1.673(2), P1–Li2 2.530(4), N1–Li3 2.037(4), N1–Li1
2.042(4), Li1–P2 2.530(4), N2–Li4 2.032(4), N2–Li2 2.038(4), Li1–H1
1.83(4), Li2–H2 1.81(4), Li3–H2 1.98(4), Li3–H1 1.96(4), Li4–H1
1.99(4), Li4–H2 1.97(4), Li1···Li2 3.131(6), Li1···Li3 2.509(5), Li1···Li4
3.051(6), Li2···Li3 3.061(6), Li3···Li3’ 2.668(8), Li3···Li4 2.821(6),
Li3’···Li4 2.691(5), Li4···Li4’ 2.682(8); H2-Li4-H1 88.3(18), Li3-H2-Li4
ca. 91.0, Li4-H1-Li4’ ca. 87.8, Li4-H1’-Li3’ ca. 89.2. Symmetry oper-
ation: #1Àx, y, Àz + 1= ; #2 Àx, Ày+1, Àz.
2
Li2···Li4···Li1 74.58(11), Li3···Li4···Li1 52.56(10).
structural determination), a hydrocarbon-soluble compound
having a central distorted (LiH)4 cube. As with other s-block
metal precursor complexes,[6a,c–e,7,8a–c] phenylsilane readily
substitutes alkyl groups with hydride ligands. When the
reaction is carried out in deuterated benzene and monitored
by multinuclear (1H, 7Li and 31P{1H}) NMR spectroscopy it is
evident that compound 2 is formed in a rapid reaction in
approximately 90% yield with PhSiH2nBu as the by-product.
[{(DipNPPh2)Li}4(LiH)4]·C6H6 (3·C6H6) crystallizes with
half a molecule in the asymmetric unit. During the course of
this study, we characterized two additional solvates,[17] each
with two full molecules of 3 in the asymmetric unit, which
have very comparable metrical features. Only the structure of
3·C6H6 will be discussed herein. The structure of 3 derives
from that of 2 by retaining the overall geometry, substituting
the nBu groups with hydride ligands, and dimerization of the
fragments through the newly formed hydride ligands. This
process leads to an Li8 cluster compound with a central
distorted (LiH)4 cube. The hydride ligands have been located
from difference maps and refined in all solvates. The Li
cations form an array of three connected edge-sharing
tetrahedrons,[21] with the middle one containing the (LiH)4
cube. All Li···Li distances fall into the range found for those of
carbon atoms. In addition, they show short Li···H contacts to
one b-methylene unit in each of the n-butyl groups (Li3 to
C50 and Li4 to C54); the shortest contacts being around
2.0 ꢀ. Some related complexes having the general formula
L2Li4nBu2 (L = anionic ligand) and featuring a distorted Li4
tetrahedron have been structurally characterized and show
similar overall features compared with those of 2.[20]
The 1H NMR spectrum of compound 2 in deuterated
benzene at 308C displays one broadened septet resonance
and two very broad doublets corresponding to the protons of
the iPr substituents. At elevated temperatures of approx-
imately 60–708C, only one sharp septet and one broadened
doublet resonance is found for those protons. Cooling a
sample of 2 in deuterated toluene leads to splitting of the
broad septet resonance at a coalescence temperature of
approximately 198C (equates to a DG° of ca. 13 kcalmolÀ1),
and at low temperatures of approximately À30 to À508C two
sharp septet and four doublet resonances are found. This
situation remains largely unchanged down to À858C, albeit
with significantly broadened resonances. At room temper-
ature, one major singlet is observed in the 7Li NMR spectrum
and the 31P{1H } NMR spectrum shows one broad resonance,
which resolves to a multiplet at low temperatures.[17] This
behavior suggests an exchange of ligands around the Li4 core
in 2, which is rapid on the NMR timescale at elevated
temperatures. Similar fluxional processes have been
observed, especially at elevated temperatures for several of
the related L2Li4nBu2 molecules.[20]
À
2. The lengths of the determined Li H bonds within the
central (LiH)4 cube (1.96(4)–1.99(4) ꢀ) are close to the
shortest Li-H distances in cubic LiH (ca. 2.03-2.04 ꢀ),[1] close
to those of [[{(Me3Si)2N}AlH2Li]3(LiH)],[11] and comparable
to those of the interstitial Li-H compounds [L6HLi8]+ and
[L6HLi7].[12,13] In addition, comparable short Li···Haliphatic
contacts are found in 3, the shortest one being around
2.0 ꢀ, and similar interactions are observed in 2. Four shorter
Li-H contacts of 1.81(4)–1.83(4) ꢀ are measured to Li1 and
Li2 of the outer tetrahedra. The hydrides, like the nBu groups
Treating [(DipNPPh2)2Li4nBu2] (2) with two equivalents
of phenylsilane at room temperature in benzene or toluene
affords the crystalline complex [{(DipNPPh2)Li}4(LiH)4] (3;
see Figure 2 for the molecular structure from a single-crystal
Angew. Chem. Int. Ed. 2012, 51, 1930 –1933
ꢀ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
1931