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J. Du et al. / Inorganic Chemistry Communications 73 (2016) 119–123
and 2, respectively. And the bond lengths of Fe1\\O are 1.918(12)–
.116(13) and 1.894(13)–2.102(15) Å for compounds 1 and 2, respec-
tively (see Tables S2 and S3). Bond valence sum (BVS) calculations
12] show all W, P, Ag, Fe atoms are in +6, +5, +1 and +3 oxidation
2
[
states in compounds 1 and 2, respectively, which are consistent with
the results of X-ray photoelectron spectroscopy (XPS) analysis (see
below). In addition, no protonated O atom was noted on the polyanions,
and H protons were added due to charge-balance considerations. As
shown in Fig. 1b, each pair of adjacent {ZP
5
W
30} polyanions are bridged
3+
2 2 2
by one [Fe(H biim)(H O) ]
subunit, forming into infinite 1D linear
chains, and further packed into a 3D supramolecular structure through
hydrogen bonding interactions (N\\H⋯O/OW 2.43(3)–3.27(4) and
2
.51(3)–3.26(3) Å for compounds 1 and 2, see Tables S4 and S5) and
electrostatic attractions (Fig. 2). The discrete protonated H biim mole-
biim]2 cations) (Fig. 2c) fill in the spaces as compensating
cations, and the results indicate that the positive charges of
2
+
cules ([H
4
[H
4
biim]2 cations are important for the formation of the final supra-
molecular network (Fig. 2a, Figs. S3–S5).
The IR spectra of {NaP 30}, {AgP 30}, compounds 1 and 2 are pre-
sented in Figs. S6 and S7. They all exhibit the characteristic vibrations of
+
5
W
5
W
−
1
the {ZP
925–918 cm ), and νas(W—Ob/c) vibrations (801–762 cm ) (O
central oxygen; O : terminal oxygen; Ob/c: bridging oxygen) [6,8]. The
5 a t
W30} polyanion: νas(P—O ) (1168–1076 cm ), νas(W–O )
−
1
−1
(
a
:
t
−
1
wide frequency ranges of 3479–3450 cm are associated to ν(O—H)
of water molecules. The weak bonds in the range of 3147–2931 cm−
1
Scheme 1. Designation and synthetic process of compound 1/2.
2
can be assigned to ν(C—H) of H biim molecules. The absorption in the
−
1
1
985 [11]. Compared with compound 1, there are two types of transi-
range of 1604–1596 cm can be regarded as the stretching vibrations
of the imidazole ring [8]. To investigate the thermal stability, thermo-
gravimetric analysis (TG/DTA) was applied, and the result curves of
compounds 1 and 2 were shown in Fig. S8. The first weight loss step
at 35 to 200 °C is 3.8% (calcd. 3.5%) for compound 1 and 3.6% (calcd.
3.5%) for compound 2, which are ascribed to the loss of all lattice
water molecules. From 200 to 1000 °C, a main weight loss of 13.3% for
compound 1 (11.9% for compound 2) corresponds to the loss of all or-
ganic composites, coordinated water molecules and sublimable phos-
+
tion metals in the structure of compound 2, one transition metal Ag
cation as a center is trapped in the inner cavity of a {AgP
5
W
30} unit,
O as a complex fragments
30} polyanion. Crystal data
and structural refinement parameters of compounds 1 and 2 were listed
in Table S1. As shown in Fig. 1a, the {ZP 30} cluster acts as a bidentate
ligand and coordinates with two [Fe(H
through the terminal oxygen atoms of two equivalent WO
3+
and two Fe ions combined with H
2 2
biim/H
are hung on the outer surface of a {AgP
5
W
5
W
3
+
2
biim)(H
2
O)
2
]
subunits
octahedra.
6
All Fe centers exhibit the same six–coordination environments, coordi-
nating with two oxygen atoms (O1W, O2W) from two coordinated
water molecules, two oxygen atoms (O38, O40) from two symmetrical
5 30
phorus oxide species originating from partly collapse of the {ZP W }
polyoxoanion skeleton. The two exothermal peaks in DTA curves ob-
served at 460 and 605 °C for compound 1 and 472 and 620 °C for com-
{
ZP
ecule (Fig. 1c). The bond lengths of Fe1\\N are in the range of
.097(15)–2.105(15) and 2.106(15)–2.110(15) Å for compounds 1
5
W
30} clusters, and two nitrogen atoms (N1, N2) from a H
2
biim mol-
2
pound 2 respectively are assigned to the combustion of the H biim
molecules and the sublimation of phosphorus oxide species [13]. In ad-
dition, there are apparent weight additions appear at 600 °C in TG
curves, which could be due to the decomposition of complex
2
3+
2 2
[Fe(H biim)(H O)
2
]
and the formation of iron oxides [14]. In order
to further verify the oxidation states of elements in the compounds,
XPS analysis was carried out. As shown in Figs. S9 and S10, the XPS spec-
tra exhibit the characteristic peaks of C 1s, N 1s, O 1s, P 2p, W 4f, Fe 2p
and Na 1s for compound 1, and the characteristic peaks of C 1s, N 1s,
O 1s, P 2p, W 4f, Fe 2p and Ag 3d for compound 2, respectively. These
results are consistent with the BVS calculation and elemental analysis,
which further confirm that all W, P, Ag and Fe atoms are in +6, +5,
+
1 and +3 oxidation states, respectively [15]. The above results indi-
cate that the {NaP 30}/{AgP 30} polyanion skeleton in compound
/2 are thermally stable at lower than 400 °C. The experimental and
5
W
5
W
1
simulated results in powder X–ray diffraction (PXRD) patterns of com-
pounds 1 and 2 are presented in Fig. S11, the main diffraction peaks po-
sitions are accordant, indicating the products are in a pure phase. The
different intensities of peaks may be caused by the diverse preferred ori-
entations of the powder samples.
The UV–Vis diffuse reflectance spectra of {NaP
compounds 1 and 2 were performed at 200–800 nm at room tempera-
ture (Fig. S12). Comparing with the spectra of parents {NaP 30} and
AgP 30}, the strong absorption bands at 265 and 350 nm of com-
5 5
W30}, {AgP W30},
5
W
{
5
W
pounds 1 and 2 respectively are assigned to the pπ → dπ charge–trans-
fer transitions of the Ob/c → W bonds (LMCT). The wide absorption
bands at 560 nm for compound 1 and 570 nm for compound 2 respec-
tively are attributed to the d–d transitions of Fe(III) [5b], indicating
Fig. 1. The polyhedral and ball–and–stick view of the coordination pattern of {ZP
the 1D chain (b) and the coordination pattern of Fe(III) (c) in compound 1/2.
5
W30} (a),