90
Y.-J. Tsai et al. / Inorganica Chimica Acta 434 (2015) 85–91
6.85 (14H, Ar–H and N–CH–N), 3.83 (br, 4H, O–CH2–CH2 in THF),
2.33 (br, 24H, Ar–CH3) 1.79 (br, 4H, CH2–CH2–CH2 in THF). 13C
NMR (CDCl3, 150 MHz, d, ppm): 167.1, 133.0, 128.3, 125.3, 122.6,
69.83, 25.25, 19.94. Anal. Calc. for C38H46N4OMg: C, 76.18; H,
7.74; N, 9.35. Found: C, 76.23; H, 7.78; N, 9.27%.
to check and solve twining problems of the crystals. The position
of the heavy atoms was determined using direct methods in the
program SHELXTL [20]. Subsequent cycles of least-squares refine-
ment followed by difference Fourier syntheses revealed the posi-
tions of the remaining non-hydrogen atoms. Non-hydrogen
atoms, excluding three carbon atoms in compound 4 were refined
with anisotropic displacement parameters, and hydrogen atoms
were added in idealized positions. Selected bond lengths, non-
bonded separations, bond angles, and torsion angles are shown
in Tables 1–4. Crystallographic data is shown in Table 5. Figures
of X-ray crystal structures of complexes 1–5 (Figs. 3–7) were gen-
erated from Ortep-3 for Windows [21] and rendered using POV-
Ray v3.6 for Windows [22].
4.5. Synthesis of [D(2-iPrPh)F]MgBr(THF)3 (4)
2.258 g of 1.0 M MesMgBr solution in THF (2.25 mmol) and
0.500 g D(2-iPrPh)FH (1.78 mmol) were mixed in 10 mL of THF at
ꢀ35 °C, giving a light yellow solution upon stirring. The mixture
was stirred overnight at room temperature, and then concentrated
down to 1.0 mL under vacuum. The resulting light yellow milky
solution with white precipitate was washed with hexanes
(3 ꢃ 1.0 mL) and dried under vacuum to give 4 as a white powder.
Isolated yield: 0.72 g, 67%. Diffusion evaporation crystallization
was set up at r.t. using the THF solution with hexanes diffusing
in, slowly producing clear block-shaped crystals suitable for X-
ray diffraction studies. 1H NMR (CDCl3, 600 MHz, d, ppm): 8.15
(s, 1H, N–CH–N), 7.21–6.87 (m, 8H, Ar–H), 3.91 (br, 12H, O–CH2–
CH2 in THF), 3.64 (sep, 2H, Ar–CH–(CH3)2), 1.84 (br, 12H, CH2–
CH2–CH2 in THF), 1.19 (d, 12H, –CH–(CH3)2). 13C NMR (CDCl3,
150 MHz, d, ppm): 166.0, 147.7, 141.7, 126.2, 125.5, 122.4, 121.3,
69.44, 27.26, 25.42, 23.53. Anal. Calc. for C31H47BrMgN2O3 (4): C,
62.06; H, 7.90; N, 4.67. Found: C, 61.86; H, 8.18; N, 4.68%.
6. Other physical measurements
Elemental analyses were performed by Complete Analysis
Laboratories, Inc., Parsippany, New Jersey. 1H and 13C NMR spectra
were acquired on a JEOL ECA-600 NMR-spectrometer (600 MHz for
1H and 150 MHz for 13C NMR) with spinning at r.t. Samples were
sealed under
a nitrogen environment before being sent for
measurements.
Acknowledgments
We thank Dr. Vyacheslav V. Samoshin for the NMR measure-
ments, Dr. Yu-Sheng Chen for his help with the single crystal mea-
surement of compound 2, and Dr. Simon J. Teat for his help with
the single crystal measurement of compound 5. We gratefully
acknowledge the support from the Department of Chemistry at
University of the Pacific, Pacific Fund and SAAG Grant at
University of the Pacific, the NSF Major Research Instrumentation
Grant (CHE-0722654) for the funding of JEOL ECA-600 NMR spec-
trometer, and the general user proposals for beam time at the
Advanced Photon Source of Argonne National Laboratory and the
Advanced Light Source of Lawrence Berkeley National Lab.
ChemMatCARS Sector 15 is principally supported by the Divisions of
Chemistry (CHE) and Materials Research (DMR), National Science
Foundation, under grant number NSF/CHE-1346572. Use of the
Advanced Photon Source, an Office of Science User Facility oper-
ated for the U.S. Department of Energy (DOE) Office of Science by
Argonne National Laboratory, was supported by the U.S. DOE under
Contract No. DE-AC02-06CH11357. The Advanced Light Source is
supported by the Director, Office of Science, and Office of Basic
Energy Sciences of the U.S. Department of Energy under Contract
No. DE-AC02-05CH11231.
4.6. Synthesis of [D(2-tBuPh)F]2Mg(THF) (5)
0.821 g of 1.0 M MesMgBr in THF (0.84 mmol) and 0.40 g
D(2-tBuPh)FH (1.30 mmol) were mixed in 10 mL of THF at
ꢀ35 °C, giving a light yellow solution upon stirring. The mixture
was stirred overnight at room temperature. Diffusion evaporation
crystallization was set up using the THF solution with hexanes dif-
fusing in at room temperature for 24 h and then at ꢀ35 °C, slowly
producing clear block-shaped crystals suitable for X-ray diffraction
studies. The resulting crystals were collected on a frit, washed with
hexanes (3 ꢃ 1.0 mL) and then dried under vacuum. Crystal yield:
0.092 g, 20%. 1H NMR (CDCl3, 600 MHz, d, ppm): 8.07 (s, 2H, N–CH–
N), 7.28 (d, 4H, Ar–H), 7.06 (t, 4H, Ar–H), 7.00 (t, 4H, Ar–H), 6.63 (d,
4H, Ar–H), 3.91 (br, 4H, O–CH2–CH2 in THF), 1.84 (br, 4H, CH2–
CH2–CH2 in THF), 1.29 (s, 36H, –C–(CH3)3). 13C NMR (CDCl3,
150 MHz, d, ppm): 166.8, 148.0, 142.2, 126.5, 126.0, 125.6, 123.1,
70.2, 35.3, 25.2, 22.7.
5. X-ray structure determinations
Crystals were carefully sealed with Teflon- and Para-film in a
capped vial and stored in a N2 filled zip-lock bag before being
shipped out for analysis. Single crystals suitable for X-ray analysis
were coated with deoxygenated Paratone-N oil and mounted on
Kaptan loops. Crystallographic data for compounds 1, 3, and 4 were
collected at 100(2) K on a Siemens (Bruker) SMART CCD area detec-
Appendix A. Supplementary material
CCDC 1058607 (1), 1058608 (2), 1058609 (3), 1058610 (4) and
1058611 (5) contains the supplementary crystallographic data for
this paper. These data can be obtained free of charge from The
tor instrument with Mo K
a radiation. Crystallographic data for
compound 2 were collected on Beamline ChemMatCARS Sector 15
at the Advanced Photon Source, Argonne National Lab using
monochromatic
radiation (k = 0.44280 Å) at
100(2) K.
Crystallographic Data for compound 5 was collected on Beamline
11.3.1 at the Advanced Light Source, Lawrence Berkeley National
Lab using monochromatic radiation (k = 0.7749 Å) at 150(2) K.
Raw data was integrated and corrected for Lorentz and polarization
effects using Bruker APEX2 v. 2009.1 [16]. Absorption corrections
were applied using SADABS [17]. Space group assignments were
determined by examination of systematic absences, E-statistics,
and successive refinement of the structures. The program PLATON
[18] was employed to confirm the absence of higher symmetry
References
for any of the crystals. The program CELL_NOW [19] was employed