Angewandte
Chemie
earth metal to form CaO and SrO cores. [L1Al(Me)] acts as a
Lewis acid and coordinates to the oxygen atoms in 7 and 8.
This type of deprotonation is the key step for generating 7 and
8.
Compound 7 is a colorless solid and 8 is a pale greenish-
yellow solid. Both are soluble in benzene, toluene, and THF.
Both 7 and 8 were characterized by NMR spectroscopy, EI
mass spectrometry, elemental analysis, and X-ray structural
analysis. The 1H NMR spectrum of 8 showed broad signals at
room temperature. Therefore, the 1H NMR spectroscopy
experiment was conducted at low temperature to give a better
Figure 2. Crystal structure of [{L1Al(Me)(m-O)Sr(thf)}2] (8); anisotropic
À
resolution of the resonances. The Al Me protons of 7 and 8
displacement parameters are shown at a 50% probability level.
Selected bond lengths [ꢃ] and angles [8] of one half of a formula unit
in the asymmetric unit: Al1–O1 1.729(3), Al1–N1 1.895(4), Al1–N2
1.906(4), Sr1–O1 2.391(3), Sr1–O2 2.324(3), Sr1–O3 2.567(3), Sr1–C3
2.787(4), C3–C5 1.348(7); O1-Sr1-O2 81.15(11), O1-Al1-N2 105.91(17),
N1-Al1-N2 96.96(17), Sr1-O1-Sr2 98.89(12), Sr1-O2-Sr3 98.66(12).
Noncoordinating THF molecules, substituents on the nitrogen atoms,
and all hydrogen atoms (except those at C5 and C35) are omitted for
clarity.
resonate at d = À1.05 and À1.06 ppm, respectively. The
signals at d = 1.58 (7) and 1.73 ppm (8) and at d = 3.98, 3.45
(7) and 3.36, 2.79 ppm (8) can be attributed to the CH3 and
CH2 groups on the L1 backbone. The IR spectra of 7 and 8
show bands at 1619 and 1624 cmÀ1, which can be assigned to
=
the C C bond. No molecular ion peaks were observed in the
mass spectra for compounds 7 and 8, but fragment ions were
detected.
Compounds 7 and 8 crystallize in the triclinic space group
P1 and the monoclinic space group Cc, respectively, both with
indicative of a single and a double bond, respectively. The
bond lengths within L1 are in the range of those known in the
¯
À
À
two molecules in the asymmetric unit (Figure 1 and
Figure 2).[10] The structures reveal the dimeric nature of
both compounds resulting in the formation of almost planar
four-membered Ca2O2 and Sr2O2 rings, which are connected
to two terminal L1AlMe units. The calcium and strontium
atoms are tetracoordinate (coordinated by one oxygen atom
of thf, one interaction to the ligand backbone, and two oxygen
literature, except for the two N C bonds (N1 C1 1.355(4),
À
À
À
N2 C3 1.395(4) (7) and N1 C1 1.354(6), N2 C3 1.410(6) ꢀ
(8)), which differ slightly from each other.[11] The two Ca O
and Sr O bond lengths in the M2O2 core are different (on
average 2.175, 2.259 (7) and 2.323, 2.394 ꢀ (8)). The longer
bonds are similar to those found in [{LCa(m-OH)(thf)}2]
À
À
(2.225(6)av ꢀ)[7]
and
[LSr(thf)(m-OH)2Sr(thf)2L]
atoms of the Al O group), and both adopt a distorted square-
(2.402(2)av ꢀ).[8]
À
planar geometry. The aluminum atoms are also tetracoordi-
nate (coordinated by two nitrogen atoms of L1, the methyl
carbon atom, and an oxygen atom) and generate two six-
membered C3N2Al rings owing to the bidentate nature of L1.
The coordination polyhedra of the aluminum atoms can best
For a detailed understanding of the electronic structure
and bonding properties of 7 and 8, we performed ab initio
density functional theory calculations as implemented in the
Gaussian 03 package.[12] We have adopted a hybrid B3LYP[13]
exchange and a correlation functional with the LANL2DZ[14]
basis set. The molecular structures from the X-ray diffraction
experiments served as the starting point for the calculations.
Since the hydrogen atom positions from the X-ray structural
determination are not comparable to the gas phase, we
relaxed all the hydrogen atoms. The calculations for natural
atomic orbitals (NAO) and natural bond order (NBO) were
performed to investigate the charge localization, bonding, and
hybridization characteristics of the structures under consid-
eration.
À
be described as highly distorted tetrahedra. The terminal C C
À
À
bond lengths in the ligand backbone (C1 C4 1.510(5), C3 C5
À
À
1.369(5) (7) and C1 C4 1.516(7), C3 C5 1.348(7) ꢀ (8)) are
We find that although the aluminum atoms of individual
rings in both 7 and 8 are surrounded by two nitrogen atoms of
the bidentate ligand L1, one methyl carbon atom, and one
oxygen atom in a slightly distorted tetrahedral fashion, the
bonding characteristics of Al show a mixture of covalent and
ionic characters with more contribution from the ionic part.
This situation is evident from the localization of charges on
the individual atoms (see the Supporting Information). The
Wiberg bond order analysis also shows a diminished cova-
lency of the bonds (Supporting Information). This ionic
character can further be argued from the molecular orbital
wave functions in Figure 3, which show the absence of
delocalization over these bonds. However, the Ca2O2 or
Sr2O2 rings in between two L1Al moieties show complete ionic
character with approximately + 1.9 e charge on each of the
Figure 1. Core structure of [{L1Al(Me)(m-O)Ca(thf)}2] (7); anisotropic
displacement parameters are shown at the 50% probability level.
Selected bond lengths [ꢃ] and angles [8] of one half of a formula unit
in the asymmetric unit: Al1–O1 1.740(2), Al1–N1 1.898(3), Al1–N2
1.900(3), Al1–C30 1.959(4), Ca1–O1 2.255(2), Ca1–O2 2.179(2), Ca1–
O3 2.415(3), Ca1–C3 2.680(3), C3–C5 1.369(5); O1-Ca1-O2 82.47(9),
O1-Al1-N2 104.24(12), N1-Al1-N2 98.14(13), Ca1-O1-Ca2 97.69(9),
Ca1-O2-Ca2 97.26(9). Noncoordinating n-hexane molecules, substitu-
ents on the nitrogen atoms, and all hydrogen atoms (except those at
C5 and C35) are omitted for clarity
Angew. Chem. Int. Ed. 2009, 48, 8740 –8742
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
8741