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L. Ding et al. / Journal of Organometallic Chemistry 637–639 (2001) 390–397
8.0 Hz, bipy-4,4%), 8.50 (d, 4H, 3J(HH)=8.0 Hz,
bipy-3,3%), 8.10 (m, 4H, bipy-5,5%), 6.03 (s, 4H, ph),
4.25, 3.95 (2×n.r., 2×4H, C5H4), 3.99 (s, 10H,
C5H5). 13C-NMR (62.9 MHz, CD3CN): l 150.9 (ph-
ipso), 146.9 (bipy-4,4%), 145.0 (bipy-2,2%), 144.9 (bipy-
6,6%), 130.0 (bipy-5,5%), 123.6 (bipy-3,3%), 122.0
(ph-CH), n.o. (C5H4-ipso), 71.7, 70.9 (C5H4), 69.1
(C5H5). FABMS of 6(PF6)2: m/z 1102 [M+; 2%], 957
[(M+−PF6); 20%], 812 [(M+−2PF6); 7%]. Anal.
Found: C, 50.33; H, 3.68; N, 5.08. Calc. for
C46H38B2F12Fe2N4O2P2 (1102.07): C, 50.13; H, 3.48;
N, 5.08.
and polarization terms; an empirical absorption cor-
rection was applied [13]. The structure was solved by
direct methods [14] and refined against F2 with full-
matrix least-squares methods [15]. Hydrogen atoms
bonded to C were calculated in ideal positions (riding
model). The hydroxyl-H atom was refined freely. A
total of 320 parameters refined, 13.9 data per parame-
ter, w=1/[|2(Fo2)+(0.0473P)2+1.8562P] where P=
(F2o+2F2c)/3, shift/error B0.001 in the last cycle of
−3
,
refinement, residual electron density +0.613 e A
/
−0.387 e A−3, R1=0.0418, wR2=0.0937 [I\2|(I)],
minimized function was ꢀw((F2o)−(Fc2))2.
,
4.5. Synthesis of 7Br and 7PF6
4.7. Crystal data of 6(PF6)2
A CH2Cl2 (60 ml) solution of 1Br (0.13 g, 0.26
mmol) was added dropwise with stirring at r.t. to
hydroquinone (0.03 g, 0.27 mmol) and NEt3 (0.03 g,
0.30 mmol) in 10 ml of CH2Cl2. The resulting mix-
ture was stirred overnight, whereupon a purple micro-
crystalline solid slowly precipitated. Insoluble material
was collected on a frit, triturated with Et2O (2×20
ml) and dried in vacuo. Yield: 0.10 g, 71%.
A red needle of 6(PF6)2 was mounted on top of a
glass filament on a CCD Diffraction System (Bruker
AXS). Final lattice parameters were obtained by
least-squares refinement of 510 reflections. Data were
collected with a crystal-to-detector distance of 40 mm
(1.78°BqB28.70°). Data were corrected for Lorentz
and polarization terms; an empirical absorption cor-
rection was applied [13]. The structure was solved by
direct methods [14] and refined against F2 with full-
matrix least-squares methods [15]. Hydrogen atoms
were calculated in ideal positions (riding model). A
total of 344 parameters refined, 18.3 data per parame-
ter, w=1/[|2(Fo2)+(0.0382P)2+0.991P] where P=
11B-NMR (64.2 MHz, Me2SO-d6): l −3.7 (h1/2
=
772 Hz). 1H-NMR (250.1 MHz, Me2SO-d6): l 9.45
(d, 2H, 3J(HH)=5.4 Hz, bipy-6,6%), 8.98 (d, 2H,
3J(HH)=8.0 Hz, bipy-3,3%), 8.87 (s, 1H, OH), 8.81
(vtr, 2H, 3J(HH)=8.0 Hz, bipy-4,4%), 8.32 (vtr, 2H,
3J(HH)=6.6 Hz, bipy-5,5%), 6.34 (d, 2H, 3J(HH)=
9.0 Hz, ph-2,6), 6.26 (d, 2H, 3J(HH)=9.0 Hz, ph-
3,5), 4.27, 4.11 (2×n.r., 2×2H, C5H4), 3.99 (s, 5H,
C5H5). 13C-NMR (62.9 MHz, Me2SO-d6): l 152.1
(ph-4), 147.3 (ph-1), 146.4 (bipy-4,4%), 144.6 (bipy-
2,2%), 144.0 (bipy-6,6%), 129.3 (bipy-5,5%), 123.2 (bipy-
3,3%), 120.9 (ph-2,6), 115.6 (ph-3,5), n.o. (C5H4-ipso),
71.1, 69.7, (C5H4), 68.2 (C5H5). Anal. Calcd. for
C26H22BBrFeN2O2 (541.03)×H2O (18.02): C, 55.86;
H, 4.33; N, 5.01. Found: C, 55.50; H, 4.35; N, 5.10.
7Br (0.07 g, 0.13 mmol) was dissolved in 20 ml of
H2O and added to an aqueous solution of NH4PF6
(0.04 g, 0.25 mmol), whereupon 7PF6 precipitated.
The precipitate was isolated by filtration, triturated
with H2O (2×10 ml) and Et2O (10 ml) and dried in
vacuo. X-ray quality crystals were grown by gas
phase diffusion of Et2O into an actonitrile solution of
7PF6 at ambient temperature.
(F2o+2F2c)/3, shift/error B0.001 in the last cycle of
−3
,
refinement, residual electron density +0.425 e A
,
−0.431 e A−3, R1=0.0601, wR2=0.0905 [I\2|(I)],
minimized function was ꢀw((F2o)−(Fc2))2.
,
4.8. Crystal data of 7PF6
A brown–black needle of 7PF6·0.5C4H10O was
mounted on top of a glass filament on a CCD Dif-
fraction System (Bruker AXS). Final lattice parame-
ters were obtained by least-squares refinement of 5419
reflections. Data were collected with a crystal-to-de-
tector distance of 40 mm (1.79°BqB25.68°). Data
were corrected for Lorentz and polarization terms; an
empirical absorption correction was applied [13]. The
structure was solved by direct methods [14] and
refined against F2 with full-matrix least-squares meth-
ods [15]. Hydrogen atoms bonded to C were calcu-
lated in ideal positions (riding model). The
hydroxyl-H atom was refined freely. A total of 376
parameters refined, 14.2 data per parameter, w=1/
[|2(Fo2)+(0.0570P)2+0.6507P] where P=(Fo2 +2F2c)/
4.6. Crystal data of 4PF6
A black needle of 4PF6 was mounted on top of a
glass filament on a CCD Diffraction System (Bruker
AXS). Final lattice parameters were obtained by
least-squares refinement of 7864 reflections. Data were
collected with a crystal-to-detector distance of 50 mm
(1.8°BqB26.02°). Data were corrected for Lorentz
3, shift/error B0.024 in the last cycle of refinement,
−3
,
residual electron density +0.720 e A
, −0.442
e A−3, R1=0.0526, wR2=0.1094 [I\2|(I)], mini-
mized function was ꢀw((F2o)−(Fc2))2.
,