Angewandte
Communications
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2
some of the most open zeolites, such as faujasite, in which the
free space is 45–50% of the crystal volume.
with decreased sizes of 2.30 2.45 nm along the a axis
(Figure 2c), in which the charge-compensated TBA cations
and guest solvent molecules are located (Figure S10). After
the removal of TBA cations and solvent molecules, the total
potential accessible volume of 3 is 71.4%, based on PLATON
calculations, which is slightly higher than that in 2.
[
13]
Variation of the reaction conditions led to the formation
of another interesting cluster organic framework 3, which is
3À
based on rhombohedral Cu I and [MnMo O L ] clusters.
2
2
6
18
2
The asymmetric unit of 3 contains one Cu I moiety and two
2
2
3À
[14]
independent [MnMo O L ] moieties, one TBA cation, and
Bond valence sum (BVS) calculations based on bond
6
18
2
one TBA moiety (Figure S8). As another conventional
cuprous iodide cluster, the Cu I cluster can be viewed as
lengths revealed that the oxidation states of Mo and Mn ions
in 1–3 are + 6 and + 3, respectively (Table S2). The average
BVS values for Cu ions in 2 and 3 are 1.155 and 1.042,
respectively, suggesting Cu ions are in the + 1 oxidation state.
These results are consistent with the charge-balanced require-
ment of the anions and the frameworks. 2 and 3 are stable in
air and the good agreement between powder X-ray diffrac-
tion (PXRD) patterns for the as-synthesized samples and the
simulated ones based on single-crystal data indicate the phase
purities of 2 and 3 (Figure S11,S12). Thermogravimetric
analyses (TGA) of 2 and 3 (Figure S13) show weight losses of
3.88% and 8.43% in 30–2408C and 30–1908C, respectively,
corresponding to the removal of free DMA (calculated as
3.52% for 2) and DEF molecules (calculated as 8.92% for 3),
respectively. As shown in Figure S11, in situ variable-temper-
ature PXRD patterns indicate that the anionic framework of
2 remains intact up to 2508C, whereas the thermal stability of
3 is lower than that of 2. 3 is only stable at temperatures lower
than 2208C, as evidenced by the variable-temperature PXRD
patterns (Figure S12), which further confirms that the frame-
work with the diamondoid topology is more stable than the
2
2
+
À
two tetrahedrally coordinated Cu ions linked by two m -I
2
anions. The Cu···Cu distance in the Cu I cluster is 2.582 ,
2
2
which is comparable with that in 2.
As shown in Figure 2a, each Cu I cluster in 3 is ligated by
2
2
3À
four pyridyl groups from four [MnMo O L ] bridges with
6
18
2
CuÀN bond lengths of 2.042(5) and 2.050(5) . Four symme-
try-related nitrogen atoms bound to the Cu I unit are
2
2
coplanar, with a N-Cu-N bond angle of 111.5(1)8, leading to
the formation of an unprecedented 2D cluster organic
framework (Figure 2b). In each layer, the coordination
3
À
connectivity between Cu2I2 clusters and [MnMo O L ]
6
18
2
anions generates giant parallelogram-shaped rings with sizes
2
of 2.46 3.05 nm (measured between opposite atoms). Each
3
À
ring is circumscribed by four Cu I and four [MnMo O L ]
2
2
6
18
2
clusters. The 2D layers are stacked in parallel along the a axis,
and each layer is slightly shifted with respect to the next one
(
4
Figure S9). The distance between the adjacent layers is about
.877 . Such stacking of the layers gives rise to 1D channels
2
D structure. In the IR spectra of 1–3 (Figure S14), the
characteristic vibrational bands of Anderson-type anions for
the terminal Mo=O units and the bridging Mo-O-Mo groups
À1
À1 [7g]
are located at 840–980 cm and 620–730 cm , respectively.
À1
The bands at 1366–1460 and 3025-2815 cm are ascribed to
[15]
the stretching vibrations of TBA cations. These results are
consistent with their single-crystal structural analyses.
The variable-temperature photoluminescent properties of
the as-synthesized framework 2 were studied in the temper-
ature range of 77–350 K (Figure 3). Upon excitation at l =
3
27 nm at 77 K, 2 exhibits a remarkable emission band with
a maximum around l = 656 nm. The emission may be
attributed to a “cluster-centered” triplet excited state that
involves both Cu and I tetrahedral units and has mixed
4
4
iodide-to-metal charge transfer and “metal-cluster-centered”
1
0
9
1
[16]
(d
Cu!d s Cu) character. As the temperature increases,
the emission intensities sharply decrease without an obvious
shift of the emission maximum, and the emission is nearly
quenched at room temperature. Such emission variation may
be attributed to the quenching effects caused by the solvent
molecules or other components gradually become stronger as
the temperature increases. The UV/Vis diffuse reflectance
spectra (Figure S15) of the polycrystalline samples showed
that the band gaps of 2 and 3 can be calculated as 2.20 and
[
17]
1
.96 eV, respectively. Pure inorganic POMs are usually
[18]
insulators,
however, the interactions between organic
ligands and the POM clusters can affect energy levels near
the Fermi level to make such hybrid POMs as potential
Figure 2. a) View of the coordination environment of the Cu I cluster
2
2
[19]
3À
semiconductors.
The magnetic susceptibility of 2 was
in 3; b) View of the 2D layer based on Cu I and [MnMo O L ]
2
2
6
18 2
measured under an applied magnetic field of 1 kOe in the
temperature range from 300 to 2 K (Figure S16). At 300 K,
clusters in 3; c) View of the 3D stacking style of 2D layers, showing 1D
channels along the a axis.
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Angew. Chem. Int. Ed. 2016, 55, 6462 –6466