X. Song et al. / Polyhedron 81 (2014) 639–645
641
cmꢁ1): 1730 (
trile: k, nm; (
eff (300 K): 4.46
CoC45
ꢂ4H
C, 50.16; H, 4.52; N, 9.34%.
m
e
@
) 1637 (
m
@
). Absorption spectrum in acetoni-
, M cm ): 194(190000), 244(49000), 327(43000).
eff (2 K): 3.69 Anal. Calc. for
O: C, 50.12; H, 4.39; N, 9.09. Found:
C
O
C
N
2
N as carrying gas. The amount of hydrogen generated was deter-
ꢁ
1
ꢁ1
mined by the external standard method. Hydrogen dissolved in the
solution was not measured and the slight effect of the hydrogen
generated on the pressure of the Schlenk bottle was neglected
for calculation of the volume of hydrogen gas.
l
l
B
.
l
B
l .
H
39
2
B F
8
N
7
O
6
2
2.6. Crystal structure determination
3
. Results and discussions
Single crystals of 1a, 1b, and 2a, suitable for X-ray diffraction
3.1. Synthesis and spectroscopic characterizations
analysis, were grown by slow diffusion of diethyl ether into the
acetonitrile solution of the complexes. The X-ray single crystal data
were collected on the Agilent Supernova Dual (Cu at zero) Atlas dif-
fractometer. Crystal data collection, refinement and reduction
were accomplished with the CrysAlisPro, Agilent Technologies,
and Version 1.171.36.28. The crystal structures were solved by
direct methods with SHELXS-97 and refined by using the SHELXL-97
crystallographic software package. All non-hydrogen atoms were
refined anisotropically. The hydrogen atoms were added in a riding
model. Details of crystal data are summarized in Table 1.
The tris(2-aminophenyl)amine can be prepared in high yield by
Pd-catalyzed reduction of tris(2-nitrophenyl) amine in the pres-
ence of hydrogen [24]. However, the reduction reaction proceeded
under the high pressure condition. In the present study, we used
hydrazine hydrate as a reducing agent to produce tris(2-aminophe-
nyl)amine without pressure vessel at ambient conditions. The
ligands L1 and L2 were made via the Schiff base condensation of
1
equiv of tris(2-aminophenyl)amine with 3 equiv of either 2-pyr-
idinecarboxaldehyde or 5-ethoxycarbonyl-2-pyridinecarboxalde-
hyde and used immediately without isolation. Complex
formation was straightforward in acetonitrile using metal salts of
2.7. Electrochemistry
2
+
2+
Co and Zn . The complexes formed quickly as evidenced by
immediate changes in the colors of the reaction mixtures and could
be isolated by concentrating the reaction mixture, followed by pre-
cipitation with diethyl ether. The obtained powders were recrystal-
lized by slow diffusion of diethyl ether and yielded the crystalline
material of red 1a, yellow 1b and red 2a, respectively. As shown in
Electrochemical measurements were made using a CH instru-
ment Model 630A electrochemical workstation. The cyclic voltam-
metry experiments were conducted on in a three electrode cell
including a glassy carbon working electrode, a Pt wire auxiliary
electrode, and a Ag/AgCl reference electrode under nitrogen atmo-
sphere. The potential was reported relative to the internal refer-
Fig. 2a, the FT-IR spectra of complexes 1a and 1b exhibit a band at
+
ence of Fc /Fc = 0.00 V. The supporting electrolyte was 0.1 M
ꢁ1
1
637 and 1633 cm , respectively, which are assigned to the
4 6
Bu NPF in acetonitrile.
stretching vibration of azomethine group (CH@N) [25]. As
expected, the FT-IR spectrum of complex 2a is very similar to that
ꢁ
1
2
.8. Photocatalysis
of 1a, except for the appearance of an intense band at 1730 cm
assigned to the stretching vibration of the C@O group. The UV–
Vis absorption spectra for the complexes shows the existence of
2 6
In a typical procedure, [Ir(ppy) (bpy)]PF (0.4 mg, 0.5 lmol), 1a
0.4 mg, 0.5 lmol) and 5 mL acetonitrile aqueous solution (1/1, v/
v) containing 10 vol% TEA were added to a Schlenck bottle. The
mixture was magnetically stirred under nitrogen atmosphere for
5 min. The system was freeze–pump-thaw degassed for three
times and then warmed to room temperature prior to irradiation.
The reaction solution was irradiated at 25 °C using a Xe lamp
300 W) with a cutoff filter (k > 400 nm). The gas phase of the reac-
(
intense absorption bands in the ultraviolet region, which may be
⁄
due to the ligand-centered
p
?
p
transitions (Fig. 2b) [15]. The
room temperature effective magnetic moments for 1a and 2a indi-
1
cate that the two complexes are of the high-spin type with three
1
0
unpaired electrons (Fig. 2c). Because of the d configuration for
Zn(II), a solid state diamagnetic moment was observed for complex
1
(
1
b, which is also confirmed by the H NMR spectrum of Zn com-
tion system was analyzed on a GC 7900 instrument with a 5 Å
molecular sieve column, a thermal conductivity detector, and using
plex 1b [13]. The data of elemental analyses agree well with the
proposed composition of the three complexes.
3.2. Description of the crystal structures
Table 1
Crystal data and structure refinement details for complexes 1a, 2a and 1b.
The crystal structures of complexes 1a, 2a and 1b are given in
Fig. 3 with selected bond lengths and angles listed in Table S1,
Complex
1aꢂ2CH
3
CN
2aꢂ2CH
3
CN
1bꢂ2CH
3
CN
which are established by means of single crystal X-ray diffraction.
Molecule formula
Formula weight
T (K)
Crystal system
Space group
a (Å)
C
40
H
33
B
2
CoF
N
8 9
C
49
H
45
B
2
CoF
8 9
N O
6
40 33 2 8 9
C H B F N Zn
878.74
100.00(10)
triclinic
ꢁ
For all three complexes, each of them consists of two BF
4
anions
872.30
99.99(14)
triclinic
P1ꢀ
12.9725(5)
13.1330(6)
13.8450(5)
79.598(3)
73.448(3)
61.917(4)
1991.79(14)
2
890
1.454
0.0737/0.1943
0.0863/0.2048
1.052
1088.49
100.01(11)
monoclinic
and a dicationic metal center that is six-coordinated by the imino-
pyridine nitrogen atoms. For complex 1a, the transoid N–Co–N
angels are in the range of 170.51–173.75° and are smaller than
the ideal 180°. The cisoid N–Co–N angels ranging from 76.34° to
P2
1
/c
P1ꢀ
15.8616(5)
13.4399(3)
23.7714(7)
90
103.168(3)
90
4934.3(2)
4
2236
12.2851(6)
13.7665(6)
13.8646(6)
83.662(4)
69.677(4)
64.512(5)
1982.74(15)
2
896
1.472
0.0480/0.1003
0.06670.1150
1.030
b (Å)
c (Å)
1
00.45° also deviate from the ideal 90° causing a slightly distorted
a
(°)
b (°)
(°)
octahedral geometry around the Co center, which is closer in
geometry to the tren-based tripodal iminopyridine cobalt complex
c
[
13,15]. An equatorial plane is defined by N(2), N(3), N(5) and N(6)
3
V (Å )
atoms, while N(4) and N(7) occupy the axial positions. The Co atom
is well located at the equatorial sphere. The Co–N bond distances
along the axis are 2.145(3) and 2.156(3) Å, which are slightly
longer than those in the mean plane (maximal value of
Z
F(000)
calc (g cm 3
ꢁ
)
r
1.465
D
R
R
1
/wR
/wR
2
(I > 2
(all data)
(I))
0.0593/0.1555
0.0697/0.1638
1.023
1
2
2
.129(3) Å). The average CoꢁNimine bond distance of 2.129(6) Å is
almost equal to the average CoꢁNpyridine bond distance of
.136(1) Å. Notably, the bridgehead nitrogen atom remains
Goodness-of-fit
GOF)
(
2