B.-L. Wu et al. / Inorganic Chemistry Communications 13 (2010) 157–159
159
unsymmetrical bridge ligand L containing biologically active group
1,3,4-oxadiazole.
Supplementary material
CCDC 743772 contains the supplementary crystallographic data
for complex 1. These data can be obtained free of charge from The
Acknowledgements
We gratefully acknowledge financial support from the National
Natural Science Foundation of China (20771094), the Science and
Technology Key Task of Henan Province (0524270061), and the
China Postdoctoral Science Foundation (20070410877).
References
Fig. 4. Solid state photoluminescent spectra of 1 (solid line) and free ligand L
(dotted line) at room temperature.
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flexibility of the ligand on the thioether moiety plays an important
role in the construction of the tubular structure. In a sense, com-
plex 1 is a helical-tube polymer with a chiral void of an opening
size about 14 Â 6 Å2 and a pitch of 7.463 Å, being dissimilar to
the triple chain polymer containing double dca-bridged chains
and the tubular polymer with the wall being similar to that of a
carbon nanotube [19–21]. Although many 1D helical polymers
and some 1D tubular architectures have been reported up to
now, the helical-tube structure in 1 constructed by a bridge ligand
spirally winding around two double-chain pillars is authentically
rare [11,12,21–23].
In the crystals, all the discrete tubular polymeric units align in
parallel along b-axis. Complementary interchain interdigitation oc-
curs with the p–p stacking interactions between 3-pyridyl groups
of the neighbouring tubes, which results in an overall 2D sheet
[Fig. 3 and S1].
[14] 5-(4-Pyridyl)-2-mercapto-1,3,4-oxadiazole and ligand
L were prepared as
described in literature [3,9,10,13]. A solution of Zn(NO3)2Á6H2O (0.0297 g,
0.1 mmol) in methanol (10 mL) was dropwise added into a solution of L
(0.0540 g, 0.2 mmol) and Nadca (0.0178 g, 0.2 mmol) in 1:1 methanol/ethanol
(20 mL) with strong stir, and then the resulting mixture was stirred at reflux
temperature for 30 min and cooled down to room temperature. After filtered
and allowed the filtrate to evaporate slowly at ambient temperature for one
month, colorless block crystals of 1 suitable for X-ray analysis were obtained
in 56% yield (based on Zn). Elemental analysis calcd (%) for C17H10N10OSZn: C
43.65, H 2.15, N 29.94, S 6.85; found: C 43.61, H 2.21, N 30.12, S 6.85. Selected
IR (KBr, cmÀ1): 3424(w), 2313(m), 2261(m), 2186(s), 1623(m), 1459(m),
1383(s), 1302(m), 834(m), 701(m), 525(m).
The electronic absorption spectra of L and 1 were respectively
recorded in methanol with a concentration of 1.0 Â 10À5 M in a
200–600 nm region using a UnicoTMUV-2102 PC UV–vis spec-
trometer at room temperature (Fig. S2). Two intense bands with
maxima at 207 and 279 nm distinctly character L, which may be
[15] X-ray crystallography: data were collected on
a
Siemens Smart CCD
radiation
diffractometer equipped with a graphite-monochromated Mo K
a
*
p ? p transition. As for
assigned to intraligand contribution of
(k = 0.71073 Å) at 291(2) K. All absorption corrections were performed using
the SADABS program. The structures was solved by direct methods and refined
by full-matrix least-squares fitting on F2 by SHELXTL-97 (G.M. Shelderic,
SHELXL-97, University of Göttingen, Germany, 1997). Crystal data for 1:
C17H10N10OSZn, orthorhombic, space group, Pnma, a = 13.125(2) Å,
b = 7.4625(13) Å, c = 19.057(3) Å, V = 1866.6(6) Å3, Z = 4, Dc = 1.657 g/cm3,
1, two stronger absorptions centered at 208 and 281 nm are
slightly bathochromic in comparison with free ligand L, which
mainly originates from
p ? p
* charge transition of L.
The photoluminescent spectra of 1 and free ligand L were mea-
sured with a Hitachi F-4500 system at room temperature. A DMF
solution of L (1.0 Â 10À4 M) excited at 308 nm emits photolumi-
nescence with a single broad band at kmax = 366 nm. When excited
at 326 nm, the emission property of solid L is very similar to that of
the DMF solution sample only with the maximum emission wave-
length undergoing a slightly blue-shift to 362 nm. The emission of
1 in solid centers at 395 nm as excited at 343 nm (Fig. 4). Although
the maximum emission wavelength of 1 undergoes a red-shift of
33 nm, the emission band is very similar to that found for free li-
gand L in terms of position and band shape. Therefore, the emission
nature of 1 is a ligand-centered emission as reported for Zn(II) or
other d10 metal complexes with N-donor ligands [24,25]. The
intensity increase of the luminescence for 1 can be explained by
the bridge coordination of L with the metal center increasing the
rigidity of L and reducing the nonradiative relaxation process.
In summary, we have successfully synthesized a novel 1D
tubular luminescent Zn(II) coordination polymer with the designed
q
calcd = 1.059 mmÀ1, R1 = 0.0860, wR2 = 0.2184 and GOF = 1.031. The positions
of H atoms were generated geometrically.
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