Inorganic Chemistry
Article
52
by the additional coordination to MN ions. Also, the
rpm at 50 °C using an a Block Bath Shaker (MyBL-100S, As One,
Japan). An aliquot (10 μL) of the reaction mixture periodically
sampled was diluted with HEPES buffer solution (pH 8.3, 100 mM,
wavenumbers of νCN similar to those of corresponding CuFe,
−1
CoFe, and GaFe appeared at 2096, 2084, and 2117 cm ,
2
,490 μL) and analyzed by a UV−vis spectrophotometer. The
II
N
respectively, supported the Fe −CN−M formation without
conversion ratio of p-NPP at a certain reaction time was determined
by the absorbance change at 400 nm ascribed to the formed p-
ligand isomerization (Figure 2). The wavenumber of ν of
GaFe-NH (2106 cm ) lower than that of GaFe (2117 cm )
by 11 cm resulted from a partial oxidation of Fe ions in GaFe
as reported previously, indicating that the valence of Fe ions
CN
−
1
−1
4
−1
−1
nitrophenolate ion (p-NP, ε = 1.57 × 10 M cm ). Recycling
performance was evaluated by adding a buffer solution containing p-
NPP to a catalyst taken out from the reaction solution by
centrifugation.
3
−
1
53
is +2 in GaFe-NH . Also, ammine ligand coordination in
3
CuFe-NH , CoFe-NH , and GaFe-NH was confirmed by the
3
3
3
−
1
RESULTS AND DISCUSSION
peaks at 1344, 1269, and 1270 cm , respectively, assigned to
H−N−H bending vibration (δ ), which was not observed
■
N
II
N
Structure of [M (H O) ] [Fe (CN) (NH )] (M Fe-NH )
HNH
2
x y
5
3
3
5
4
−1
II
II
III
N
for CuFe, CoFe, and GaFe. The peaks at around 1400 cm
observed for CuFe-NH , CoFe-NH , and GaFe-NH can be
Complexes. Cu , Co , and Ga ions were chosen as M ions
of the CN-deficient PBAs because of different valence and
3
3
3
+
II
assigned to δHNH of ammonium ion (NH ) trapped in the
4
54
catalytic behavior of each meal ion as reported previously. Cu
ion is a divalent ion with low activity for the hydrolysis of p-
+
interstitial sites of PBAs. NH4 could be formed by partial
replacement of NH to H O ligands during synthesis in an
II
nitrophenyl phosphate (p-NPP); Co ion is also divalent but
3
2
III
aqueous solution (vide infra).
catalytically active, and Ga is trivalent and catalytically
2
8
II
II
Measurements of nitrogen (N ) adsorption−desorption
active. [Cu (H O)
]
[Fe (CN) (NH )] (CuFe-NH ),
2
2
8/3 3/2
II
5
3
3
II
isotherms of PBAs were performed to investigate their porous
structures (Figure S4). The total surface areas were calculated
from the Brunauer−Emmett−Teller (BET) method (Table 1).
[
[
Co (H O)8/3] [Fe (CN) (NH )] (CoFe-NH ), and
Ga (H O)][Fe (CN) (NH )] (GaFe-NH ) were obtained
by the reaction of Na [Fe (CN) (NH )] with Cu , Co , and
Ga ions, respectively. Similarly, [Cu (H O) ] [Fe (CN) ]
CuFe), [Co (H O) ] [Fe (CN) ] (CoFe), and
Ga (H O)
the reaction of K [Fe (CN) ] with the corresponding metal
2
3/2
II
5
3
3
III
2
5
3
3
II
II
II
3
5
3
III
II
II
2
3 2
6
II
II
Table 1. Total Surface Areas Obtained by the Brunauer−
Emmett−Teller (BET) Method and Pore Diameters
Obtained by the Microporous (MP) Method and the
Barrett−Joyner−Halenda (BJH) Method of a Series of
(
[
2 3 2 6
III
II
] [Fe (CN) ] (GaFe) were synthesized by
3/2 4/3 6
2
II
4
6
ions. The scanning electron microscope (SEM) images showed
and most of the particles were less than 20 μm (Figure S1). No
shape-controlled particles were observed even at smaller
particles. Insignificant contamination of Na and K ions in
the PBAs was assured by inductively coupled plasma optical
emission spectroscopy (ICP-OES) and X-ray fluorescence
PBAs Calculated from Their N Adsorption-Desorption
2
Isotherms
BET surface area,
micropore
diameter, nm
mesopore
diameter, nm
+
+
2
−1
PBA
m g
CuFe-NH3
CuFe
77
101
32
0.7
0.7
0.7
0.7
0.7
0.6
0.8
7.0
10.2
4.6
5.3
10.8
3.2
CuFe-H O
2
CoFe-NH3
CoFe
GaFe-NH3
GaFe
50
284
179
393
X-ray photoelectron spectroscopy (XPS) measurements of
3
3.5
of Cu 2p, Fe 2p, O 1s, and N 1s (Figure S3). The values for
binding energy of Cu 2p3/2 of CuFe-NH and CuFe were
3
9
33.8 and 933.2 eV, respectively, which are close to the typical
Homogeneous distribution of micropores (0.6−0.8 nm)
formed by the cubic lattice structures of PBAs were evidenced
by the microporous (MP) method. Type IV isotherms
observed for a series of PBAs suggested the presence of
mesopores in the sizes of 3−11 nm as determined by the
Barrett−Joyner−Halenda (BJH) method. The mesopores in
this size range are formed by the gaps among PBA particles, as
II
50
values for the Cu species (933.5 eV). The binding energies
of Fe 2p3/2 peaks were found at 708.7 and 709.1 eV for CuFe-
NH and CuFe, respectively, which are also comparable to the
3
II
50
typical binding energy of Fe species (709.1 eV). These
results suggest that the involvement of NH ligands hardly
3
II
II
affected the oxidation states of Cu and Fe ions. The binding
28
energy of O 1s in CuFe-NH was 532.5 eV, which is virtually
reported previously.
3
the same to that of CuFe (532.2 eV). The binding energy of N
The powder X-ray diffraction (PXRD) patterns obtained for
N
1
s in CuFe-NH (397.9 eV) was also similar to that in CuFe
M Fe-NH complexes were assignable to a cubic structure
3
3
N
(
398.3 eV) even in the presence of NH ligands because the
(Figure 3a, c, e). The cell parameters obtained for M = Cu,
3
−
peaks for N 1s in CN and NH ligands (397.7 and 399.0 eV,
Co, and Ga were a = 10.00, 9.94, and 10.04 Å, respectively.
The a values were comparable to those of corresponding
3
respectively, according to the literature) are severely over-
5
1
N
II
lapped.
M Fe complexes without open sites on Fe ions, where a =
II
N
N
N
The bridging structures of Fe −CN−M in M Fe-NH3
complexes were confirmed by infrared (IR) spectroscopy. The
CN-stretching bands (νCN) of CuFe-NH , CoFe-NH , and
9.95, 10.10, and 10.02 Å for M = Cu, Co, and Ga, respectively
(Figure 4b, d, f). Broad peaks observed for M Fe-NH3
N
complexes, especially for GaFe-NH , compared with those of
3
3
3
−
1
N
GaFe-NH3 appeared at 2094, 2084, and 2106 cm ,
M Fe complexes resulted from the low crystallinity due to
local disorder originated from partial deficiencies of CN
ligands of M Fe-NH complexes, or from small crystallite
−
respectively, which were shifted from that of
II
−1
N
K [Fe (CN) (NH )] (2038 cm ) in the higher wavenumber
3
5
3
3
region (Figure 2). Such higher wavenumber shift evidenced
even with maintaining high crystallinity. The high wavenumber
shift of νCN in IR spectra and the presence of microporous
structures evidenced by the N2 adsorption−desorption
II
N
the formation of Fe −CN−M structures, as the electron
−
density of an antibonding orbital of CN ligand was reduced
D
Inorg. Chem. XXXX, XXX, XXX−XXX