P. Shukla et al. / Journal of Organometallic Chemistry 690 (2005) 1366–1371
1367
we explore the use of ligand 3 (Ar = p-fluorophenyl) in
the context of aluminum chemistry.
least squares on F2 using the Siemens SHELX PLUS 5.0
(PC) software package [9]. All non-hydrogen atoms
were allowed anisotropic thermal motion and all hydro-
gen atoms, which were included in calculated positions
˚
2. Experimental
(C–H 0.96 A), were refined using a riding model and a
general isotropic thermal parameter. The crystal and
structure refinement details are presented in Table 1.
2.1. General
All manipulations and reactions were performed un-
der a dry, oxygen-free, catalyst-scrubbed argon atmo-
sphere using standard Schlenk techniques or under a
dry, oxygen-free, helium atmosphere in a Vacuum
Atmospheres drybox. All glassware was oven-dried
and vacuum- and argon flow-degassed before use. Tolu-
ene and diethyl ether were distilled under N2 from so-
dium benzophenone ketyl and degassed prior to use.
The syntheses of the ligands are described in a previous
paper [8]; Me2AlCl and AlCl3 were purchased from
commercial sources and used without further
purification.
2.4. AlCl[OC(Me)CHC(Me)N(p-C6H4F)]2 (4)
2.4.1. Method 1
A solution of n-BuLi (2.56 mmol) in hexanes was
added slowly to
a
solution of O@C(Me)CH@
C(Me)N(H)(p-C6H4F) (0.50 g, 2.56 mmol) in 20 ml of
diethyl ether at 0 ꢁC. The reaction mixture was allowed
to come to room temperature over a period of 3 h, after
which time the volatiles were removed in vacuo. The
‘‘O@C(Me)CH@C(Me)N(Li)(p-C6H4F)’’ in 70 ml of
diethyl ether was added slowly to a solution of AlCl3
(0.34 g, 2.55 mmol) in 20 ml of diethyl ether at 0 ꢁC.
The reaction mixture was allowed to come to room tem-
perature and stirred overnight, after which time the vol-
atiles were removed in vacuo, and the resulting pale
yellow residue was extracted with toluene (75 ml). After
filtration through a glass frit covered with a pad of dia-
tomaceous earth, the yellow filtrate was concentrated
and maintained at ambient temperature for 1 week
which resulted in the formation of a crop of colorless
crystals of 4 (0.02 g, 2% yield, m.p. 118–124 ꢁC). 1H
NMR (C6D6, 25 ꢁC): d 7.1 (m, 8H, w1/2 = 30 Hz, aryl-
ring protons), 5.4 (s, 2H, CH), 2.2 (s, 6H, CH3CN),
2.0 (s, 6H, CH3CO). 19F NMR (CDCl3, 25 ꢁC): d
ꢀ118.0 (m, w1/2 = 12 Hz). 27Al NMR (C6D6, 25 ꢁC): d
91 (broad, w1/2 = 100 Hz). MS (CI+, CH4): m/e 447
(M + H), 411 (M ꢀ Cl), 194 [O@C(Me)CH@C(Me)-
N(H)(p-C6H4F) + H]. HRMS (CI, CH4) Calc. for
C22H22AlClF2N2O2: 447.123154. Found: 447.122689.
2.2. Physical measurements
Low-resolution CI mass spectra were obtained on a
Finnigan MAT TSQ-700 mass spectrometer, and high-
resolution CI mass spectra were measured on a VG
Analytical ZAB-VE sector instrument. All MS analyses
were performed on samples that had been sealed in glass
capillaries under argon in a drybox. Solution-phase
NMR spectra were recorded at 298 K on a GE Varian
Unity 300 instrument (1H, 300 MHz; 19F, 282 MHz;
27Al, 78 MHz) at the University of Texas at Austin or
the Los Alamos National Laboratory (LANL). All
NMR samples were run immediately following removal
from the drybox. Benzene-d6 and chloroform-d were
vacuum distilled under argon from sodium benzophe-
1
none ketyl prior to use. The H NMR chemical shifts
are reported relative to tetramethylsilane (d 0.00) and
referenced to solvent. The 19F NMR chemical shifts
are reported relative to freon-11 (d 0.00) and referenced
to C6H5CF3 (d ꢀ63.5 at LANL) or to freon-11 (d 0.00 at
UT-Austin). The 27Al NMR chemical shifts are reported
relative to [Al(H2O)6]3+ (d 0.00).
2.4.2. Method 2
A solution of O@C(Me)CH@C(Me)N(H)(p-C6H4F)
(0.32 g, 1.63 mmol) in 3 ml of toluene was added to a
solution of Me2AlCl (0.15 g, 1.62 mmol) in 3 ml of tolu-
ene. Following the cessation of gas evolution, the reac-
tion mixture was stirred overnight at ambient
temperature. Crystals of 4 formed upon slow evapora-
tion of the solvent. (0.12 g, 33% yield). The spectro-
scopic data were identical with those listed above for
Method 1.
2.3. X-ray structure determination of complexes 4 and 5
Crystals of suitable quality were collected under an
argon atmosphere from Schlenk-type flasks, and cov-
ered immediately with degassed perfluorinated polyether
oil. The X-ray data were collected on a Nonius Kappa
CCD diffractometer at 153 K using an Oxford Cryo-
stream low-temperature device and graphite-monochro-
2.5. [AlCl2{O@C(Me)CH@C(Me)N(H)(p-C6H4F)}4]-
[AlCl4] (5)
˚
mated Mo Ka radiation (k = 0.71073 A). A correction
was applied for Lorentz polarization. All structures were
solved by direct methods, and refined by full-matrix
The solution from which the crystals of 4 were grown
(by Method 1) was transferred to a separate Schlenk
flask. The solvent was removed in vacuo and the yellow