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L. Yi et al. / Inorganic Chemistry Communications 6 (2003) 1209–1212
was kept at 0 °C for 3 days. The colorless crystalline
products suitable for X-ray structure analysis were
gradually formed in the solution. Anal. Calc. for
C48H38Cl8N18O9Zn (1): C, 42.36; H, 2.79; N, 18.53%;
Found: C, 42.10; H, 2.82; N, 18.45%. m.p.: 235–237 °C.
Anal. Calc. for C16H12Cl4N6Zn (2): C, 38.75; H, 2.42;
N, 16.95%; Found: C, 38.62; H, 2.50; N, 16.80%. m.p.:
217–219 °C.
2.2. Physical measurements
All the solvents and chemicals were reagent grade and
used without further purification. Elemental analyses of
carbon, hydrogen and nitrogen were carried out with a
Perkin–Elmer analyzer model 240. Infrared spectra were
measured on a Bruker Vector 22 FT-IR instrument from
KBr pellets. Diffuse reflectance absorption spectrum was
performed with a Shimadzu UV-2101PC spectropho-
tometer in the range of 200–2000 nm at room temper-
ature. The photoluminescence spectrum was measured
by MPF-4 fluorescence spectrophotometer with a xenon
arc lamp as the light source.
Fig. 1. The ORTEP drawing of [Zn(pCltrz)6]2þ. Selected interatomic
ꢀ
bond distances (A) and angles (°): Zn(1)–N(13) 2.132(4), Zn(1)–N(4)
2.156(4), Zn(1)–N(10) 2.175(3), Zn(1)–N(16) 2.177(4), Zn(1)–N(7)
2.202(4), Zn(1)–N(1) 2.221(4), N(13)–Zn(1)–N(4) 176.51(14), N(13)–
Zn(1)–N(10) 90.32(14), N(13)–Zn(1)–N(16) 90.01(14), N(16)–Zn(1)–
N(7) 179.17(14), N(13)–Zn(1)–N(7) 90.72(14), N(10)–Zn(1)–N(16)
89.15(14), N(13)–Zn(1)–N(1) 88.06(14).
2.3. Crystal structure determination
Crystal data for 1: C48H38Cl8N18O9Zn, M ¼ 1359:93,
monoclinic, P21=c, a ¼ 20:369ð12Þ, b ¼ 14:773ð8Þ, c ¼
The N(13)–Zn(1)–N(4), N(13)–Zn(1)–N(16) and N(13)–
Zn(1)–N(10) angles are 176.51(14), 90.01(14) and 90.32
(14)°, respectively, indicating a slight distortion. It is
noticeable that there is a considerable variation in the
Zn–N distances around the metal ion and Zn(1)–N(13)
3
ꢀ
ꢀ
20:416ð12Þ A, b ¼ 113:675ð8Þ°, V ¼ 5627ð6Þ A , Z ¼ 4,
Dc ¼ 1:605 g/cm3, R1 ¼ 0:0447, wR2 ¼ 0:0988 (I > 2rðIÞ);
R1 ¼ 0:1010, wR2 ¼ 0:1345 (for all data), and S ¼ 0:898.
Crystal data for 2: C16H12Cl4N6Zn, M ¼ 495:49, mono-
ꢀ
clinic, P21=c, a ¼ 14:892ð5Þ, b ¼ 18:594ð7Þ, c ¼ 7:147ð2Þ
bond length is almost 0.09 A shorter than Zn(1)–N(7)
3
ꢀ
ꢀ
A, b ¼ 99:000ð6Þ°, V ¼ 1954:7ð11Þ A , Z ¼ 4, Dc ¼ 1:684
g/cm3, R1 ¼ 0:0423, wR2 ¼ 0:0864 (I > 2rðIÞ); R1 ¼
0:0959, wR2 ¼ 0:1297 (for all data), and S ¼ 0:900. X-ray
diffractions were collected on a BRUKER SMART 1000
CCD detector with graphite-monochromatized Mo-Ka
distance, this may be due to the need to ÔeaseÕ the space
repulsion of the triazole ligands. Through a few
mononuclear compounds are known in which the 4-
substituted triazole coordinates through N1 [17–20],
this is the first example that metal ion coordinated via
six triazole ligands. The ORTEP of 2 is shown in Fig. 2
together with the atomic labeling scheme. The coordi-
nation sphere of the Zn(II) ion may be described as a
slightly distorted tetrahedron. The metal ion in 2 is
coordinated by two nitrogen atoms of two triazole li-
gands and two chloride atoms. The Zn–N bond lengths
are very close to each other with the average value of
ꢀ
radiation with radiation wavelength 0.71073 A at 293(2)
K. The structures were solved by direct-methods using the
program SHELXS-97 [15] and Fourier difference tech-
niques, and refined by full-matrix least-squares method
on F 2 using SHELXL 97 [16].
ꢀ
3. Results and discussion
2.018 A. The Zn–Cl distances are 2.2039 (17) and
ꢀ
2.2352 (18) A, respectively. The bond angles around the
Two zinc salts, Zn(ClO4)2 ꢀ 6H2O as species with non-
coordinating anions and ZnCl2 as species with coordi-
nating anions, were chosen for the reactions with pCltrz.
The structures of 1 and 2 have shown that the coordi-
native behaviour of the anions was as expected [17].
The cationic unit of 1 is depicted in Fig. 1. The
zinc(II) ion in 1 is located on a slightly distorted oc-
tahedral center relating six N-donating pCltrz ligands.
zinc atom deviate much with respect to the value ex-
pected for an ideal tetrahedron, 109.4°. Compared with
1, the dihedral angle between phenyl ring and triazole
ring of the pCltrz ligand is almost 4° bigger in com-
pound 2, this may attribute to the space repulsion li-
gands in 1.
The excitation and emission spectra of pure 1, 2 and
pCltrz in the DMF solution with the same concentra-
tion at room temperature are shown in Fig. 3. The very
strong blue fluorescence for the two complexes can be
ꢀ
The Zn–N (2.132(4)–2.221(4) A) distances are within
the range observed for other octahedral complexes [17].