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fascinating structures [7–11]. Especially, the flexible 1,4-bis(1,2,4-
triazol-1-ylmethyl)-benzene (btx) not only possesses the merits of
triazole, but can also freely bend and rotate to interact with metal
ions. [12–14]. A series of Cd–btx complexes with the third-order
NLO (nonlinear optics) properties and Co-btx coordination poly-
mers with novel topologies have been studied [15,16]. In addition,
aromatic carboxylates such as 1,2,4,5-benzenetetracarboxylate,
1,3,5-benzenetricarboxylate, terephthalate, 5-substituted iso-
phthalate, ligands are of particular interest due to their multi-car-
boxylate groups and the versatile coordination modes of these
carboxylate groups, such as monodentate, bis-monodentate or
chelating modes, leading to diverse structures of the resulting
MOCPs [17]. The combination of flexible btx and aromatic polycar-
boxylate ligands may induce novel architectures and versatile
properties. Wang and co-workers have presented a rare example
of entangled coordination polymer containing both interpenetrat-
ing and polythreading features coordination polymer [Zn(CH3O-
ip)(btx)]2ÁH2O (CH3O-ip = 5-methoxyisophthalate) [18]. We have
reported three unprecedented binodal high-connected metal–
organic frameworks constructed from btx and 1,2,4,5-benzenetet-
racarboxylate [19,20]. As a part of our ongoing studies on ternary
transition metal complexes based on btx and aromatic carboxylate
ligands, two new coordination polymers with interesting
luminescence properties were prepared and structurally character-
ized. [Ni(btx)(nip)(H2O)]n (1) (H2nip = 5-nitroisophthalic acid,
H2mip = 5-methyisophthalic acid) reveals a 3-fold interpenetrating
3D CdSO4-type network, while {[Cd(btx)(mip)(H2O)]ÁH2O}n (2)
shows a 2D (4, 4) sheet-like network, which is finally extended into
a 3D 3,5T1 supramolecular framework through multiple strong
hydrogen bond interactions. To the best of our knowledge, coordi-
nation polymers exhibiting such 3,5T1 supramolecular network
have only rarely been reported [21].
{[Cd(btx)(mip)(H2O)]ÁH2O}n (2)
The synthetic procedure of 2 was analogous to the synthesis of
1, except that H2nip and Ni(CH3COO)2Á4H2O were used instead of
H2mip (0.1 mmol, 18.0 mg) and Cd(CH3COO)2Á2H2O (0.1 mmol,
26.7 mg), respectively. Colorless block-shaped crystals of 2 (yield:
43%) could be obtained. Anal. Calcd. for C21H22CdN6O6 (%): C,
44.50, H, 3.91, N, 14.83. Found (%): C, 44.36, H, 3.82, N, 14.55. IR
(KBr, cm–1): 3427(vs), 3103(w), 2948(w), 1640(s), 1542(s),
1483(s), 1348(s), 1284(w), 1064(s), 733(w), 683(w).
X-ray crystallography
The crystallographic data for the single crystal of compound 1
was collected at 100 K on an Agilent SuperNova Dual Source dif-
fractometer with Atlas CCD detector, microfocus sources and
focusing multilayer optics, using Mo K
a radiation (k = 0.71073 Å).
CrysAlis PRO [23] software was used to collect, index, scale and ap-
ply analytical absorption correction based on faces of the crystal
with multi-scan mode. X-ray diffraction data for 2 was collected
on a Bruker Smart 1000 CCD diffractometer using graphite-mono-
chromated Mo K
a radiation (k = 0.71073 Å) at room temperature
with -scan mode. A semi-empirical absorption correction was ap-
x
plied using the SADABS program [24]. Both structures were solved
by direct methods with SHELXS-97 and refined by full-matrix least
squares on F2 with SHELXTL [25]. All non-hydrogen atoms were re-
fined with anisotropic thermal parameters. The H-atoms of organic
ligands were generated theoretically onto the specific atoms and
refined isotropically. The aqua hydrogen atoms in 1 and 2 were lo-
cated from difference Fourier maps and refined with isotropic dis-
placement parameters. The crystallographic data for 1 and 2 are
listed in Table 1, and selected length and angle parameters for 1
and 2 are presented in Table 2, respectively.
Results and discussion
Experimental
Crystal structures
Materials and measurements
Crystal structures of compound 1
The structure of 1 is a 3D MOF. X-ray analysis reveals that 1
crystallized in the monoclinic space group Cc. The asymmetric unit
All reagents were obtained from commercial sources and used
without further purification. The ligand btx was prepared accord-
ing to literature procedures [22]. Elemental analysis (C, H, and N)
was performed on a Perkin–Elmer 240C Elemental Analyzer. Power
X-ray diffraction (XRD) data were recorded on a Rigaku D/Max-
2500 diffractometer at 40 kV, 100 mA for a Cu-target tube and a
graphite monochromator. FT-IR spectra were recorded on an
Avatar 360 (Nicolet) spectrophotometer between 400 and
Table 1
Crystal and refinement data for complexes 1 and 2.
1
C
2
Empirical formula
Formula weight
Crystal system
Space group
a (Å)
20H17N7NiO7
C21H22CdN6O6
566.85
Triclinic
4000 cm–1
, using the KBr pellet method. Thermogravimetric
526.12
Monoclinic
Cc
16.1760(3)
16.9691(3)
7.3806(2)
90
analyses (TGA) were conducted on a Netzsch TG 209 thermal ana-
lyzer in N2 environmental at a heating rate of 10 °C/min up to
800 °C. The fluorescence spectra were collected with a Hitachi
F-4500 spectrophotometer at room temperature.
Pı
¯
10.2021(7)
11.4351(8)
11.8614(8)
69.2300(8)
68.8065(8)
67.0920(7)
1150.98(14)
2
b (Å)
c (Å)
a
(deg)
b (deg)
94.459(2)
90
2019.77(7)
4
1.730
1.025
c
(deg)
Preparation of the complexes 1 and 2
[Ni(btx)(nip)(H2O)]n (1)
V (Å3)
Z
Dcalc (g/m3)
1.636
0.999
572
(mm–1
)
A
mixture of Ni(CH3COO)2Á4H2O (0.1 mmol, 24.9 mg), btx
l
(0.1 mmol, 24.0 mg), H2nip (0.1 mmol, 105.5 mg) was added in
20 mL H2O. It was then sealed in a 25 mL Teflon-lined stainless
steel autoclave and heated at 160 °C for 3 days; then, the reaction
system was cooled to room temperature at 5 °C/h. Green block-
shaped crystals were collected by filtration and washed with dis-
tilled water in 45% yield (based on Ni(CH3COO)2Á4H2O). Anal.
Calcd. for C20H17N7NiO7 (%): C, 45.66, H, 3.26, N, 18.64. Found
(%): C, 45.32, H, 3.12, N, 18.39. IR (KBr, cm–1): 3420(vs), 3120(w),
2368(w), 1617(s), 1532(s), 1461(s), 1353(s), 1282(s), 1125(w),
733(w), 677(w).
F(000)
1080
Crystal size (mm)
Total reflections
Unique reflections
Rint
0.28 Â 0.21 Â 0.15
21,862
4784
0.0635
0.851
0.27 Â 0.23 Â 0.22
7039
5062
0.0164
1.002
0.0254
0.0622
0.341
–0.421
GOF
R1 (I > 2
r
(I))
0.0366
0.0805
0.393
wR2 (I > 2
r(I))
D
D
q
q
max (eÅ–3
min (eÅ–3
)
)
–0.330
[w F2o À F2c 2]/
R
[w F2o
]
.
2
1/2
R1
=
R
||Fo|–|Fc||/
R
|Fo|; wR2
=
R