A R T I C L E S
Tondreau et al.
hemisphere routine was used for data collection and determination
of lattice constants. The space group was identified and the data
were processed using the Bruker SAINT+ program and corrected
for absorption using SADABS. The structures were solved using
direct methods (SHELXS), completed by subsequent Fourier
synthesis, and refined by full-matrix least-squares procedures.
Quantum-Chemical Calculations. All DFT calculations were
performed with the ORCA program package.63 The geometry
optimizations of the complexes and single-point calculations on
the optimized geometries were carried out at the B3LYP level64-66
of DFT. This hybrid functional often gives better results for
transition metal compounds than pure gradient-corrected functionals,
especially with regard to metal-ligand covalency.67 The all-electron
Gaussian basis sets were those developed by the Ahlrichs group.68,69
Triple-ꢁ-quality basis sets TZVP with one set of polarization
functions on the metal and on the atoms directly coordinated to
the metal center were used.69 For the carbon and hydrogen atoms,
slightly smaller polarized split-valence SV(P) basis sets were used
that were of double-ꢁ quality in the valence region and contained
a polarizing set of d-functions on the non-hydrogen atoms.68
Auxiliary basis sets used to expand the electron density in the
resolution-of-the-identity (RI) approach were chosen70-72 to match
the orbital basis.
The SCF calculations were tightly converged (1 × 10-8 Eh in
energy, 1 × 10-7 Eh in the density change, and 1 × 10-7 in
maximum element of the DIIS error vector). The geometry
optimizations for all complexes were carried out in redundant
internal coordinates without imposing symmetry constraints. In all
cases, the geometries were considered converged after the energy
change was less than 5 × 10-6 Eh, the gradient norm and maximum
gradient element were smaller than 1 × 10-4 and 3 × 10-4 Eh
bohr-1, respectively, and the root-mean-square and maximum
displacements of all atoms were smaller than 2 × 10-3 and 4 ×
10-3 bohr, respectively.
CP(PPP) basis set78 for iron. The Mo¨ssbauer isomer shifts were
calculated from the computed electron densities at the iron centers
as previously described.79
Preparation of [Li(Et2O)3][(iPrPDI)Fe(CH2CMe3)N2]. A 50 mL
round-bottom flask was charged with 0.150 g (0.25 mmol) of
(iPrPDI)Fe(N2)2 and approximately 20 mL of diethyl ether. The
contents of the flask were cooled to -35 °C. A scintillation vial
was charged with 0.020 g (0.25 mmol) of neopentyl lithium and
approximately 10 mL of diethyl ether, and the resulting solution
was cooled to -35 °C. The flask containing the iron compound
was stirred, and the neopentyl lithium solution was added dropwise
over the course of 5 min. The reaction was warmed to room
temperature and stirred. After 0.5 h, the reaction mixture was filtered
through Celite. The filtrate was collected, and the volatiles were
removed. The resulting residue was dissolved in a minimal amount
of diethyl ether, and the resulting solution was placed in a
scintillation vial and cooled overnight at -35 °C for recrystalliza-
tion. The resulting solid was collected on a glass frit and yielded
0.078 g (34%) of [Li(Et2O)3][(iPrPDI)Fe(CH2CMe3)(N2)]. Analysis
for C50H84N5FeO3Li, calcd: C, 69.34; H, 9.78; N, 8.09. Found: C,
69.73; H, 8.92; N, 8.84. Magnetic susceptibility (benzene-d6, 23
°C): µeff ) 0 µB. IR (KBr): ν(N2) ) 1948 cm-1
.
Alternative Preparation of [Li(Et2O)3][(iPrPDI)Fe(CH2CMe3)-
(N2)]. This molecule was prepared using a procedure identical to
that described above, with the exception that 0.100 g (0.14 mmol)
of (iPrPDI)FeBr and 0.022 g (0.28 mmol) of neopentyl lithium
were used as the reagents. Recrystallization from diethyl ether at
-35 °C furnished 0.052 g (41%) of [Li(Et2O)3][(iPrPDI)Fe-
(CH2CMe3)(N2)].
Preparation of [Li(12-Crown-4)][(iPrPDI)Fe(CH2CMe3)(N2)].
A scintillation vial was charged with 0.05 g (0.06 mmol) of
[Li(Et2O)3][(iPrPDI)Fe(CH2SiMe3)(N2)] and approximately 5 mL of
diethyl ether. A solution containing 0.02 g (0.12 mmol) of 12-
crown-4 in diethyl ether was added to the stirring solution of iron
compound. The volume of the solution was reduced to ap-
proximately 5 mL, and the vial was placed in a -35 °C freezer.
The solvent was decanted, and the solid was dried under reduced
pressure to yield 0.030 g (64%) of a dark red-brown solid, identified
as [Li(12-Crown-4)][(iPrPDI)Fe(CH2CMe3)(N2)]. Analysis for
C46H70N5FeO4Li, calcd: C, 67.39; H, 8.61; N, 8.54. Found: C, 67.06;
H, 8.42; N, 8.34. Magnetic susceptibility: µeff ) 0 µB. IR (KBr):
Throughout this paper we describe our computational results by
using the broken-symmetry (BS) approach described by Ginsberg73
and Noodleman.74 Because several BS solutions to the spin-
unrestricted Kohn-Sham equations may be obtained, the general
notation BS(m,n)75 has been adopted, where m (n) denotes the
number of spin-up (spin-down) electrons at the two interacting
fragments. Canonical and corresponding76 orbitals as well as spin
density plots were generated with the program Molekel.77 Non-
relativistic single-point calculations on the optimized geometries
were carried out to predict Mo¨ssbauer spectral parameters (isomer
shifts and quadrupole splittings). These calculations employed the
ν(N2) ) 1996 cm-1
.
Attempted Preparation of [Li(Et2O)3][(iPrPDI)Fe(CH2SiMe3)-
(N2)]. Attempts to synthesize this compound were carried out using
the methods described above to successfully prepare
[Li(Et2O)3][(iPrPDI)Fe(CH2CMe3)(N2)]. In a typical experiment,
0.300 g (0.50 mmol) of (iPrPDI)Fe(N2)2 and 0.047 g (0.53 mmol)
of LiCH2SiMe3 were used. Recrystallization from diethyl ether at
-35 °C furnished 0.24 g (51%) of red crystals, identified as
(iPrPDI)Fe(CH2SiMe3), containing about 5% (as judged by Mo¨ss-
bauer spectroscopy) of the desired [Li(Et2O)3][(iPrPDI)Fe-
(63) Neese, F. Orcasan ab initio, DFT and Semiempirical Electronic
Structure Package, Version 2.7, Revision 0; Institut fu¨r Physikalische
und Theoretische Chemie, Universita¨t Bonn: Bonn, Germany, August
2009.
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(CH2SiMe3)(N2)]. IR (KBr): ν(N2) ) 1938 cm-1
.
Preparation of [(iPrPDI)Fe(CH2CMe3)][BPh4]. A 20 mL scin-
tillation vial was charged with 0.100 g (0.164 mmol) of
(iPrPDI)Fe(CH2CMe3), 0.083 g (0.164 mmol) of [Cp2Fe][BPh4], and
a stir bar. Approximately 7 mL of benzene was added to the mixture
of solids with stirring. The stirring rate was increased as the reaction
mixture thickened and a precipitate formed. After 5 min, an equal
volume of pentane was added, and the stirring was continued for
another 10 min. The solid was collected on a glass frit and washed
four times with ∼20 mL of pentane. The solid was dried under
vacuum and yielded 0.143 g (93%) of a dull gray-red powder,
identified as [(iPrPDI)Fe(CH2CMe3)][BPh4]. Analysis for
C62H74N3FeB, calcd: C, 80.25; H, 8.04; N, 4.53. Found: C, 80.41;
H, 7.84; N, 4.21. Magnetic susceptibility (MSB, 23 °C): µeff ) 4.8
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