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Y. Wei et al. / Inorganic Chemistry Communications 10 (2007) 910–913
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chains linked by carboxylate array conformably toward
5.5
5.0
4.5
4.0
3.5
3.0
2.5
2.0
1.5
one direction in the three-dimensional network.
80
60
40
20
0
Acknowledgement
We gratefully acknowledge the financial support of Nat-
ural Science Foundation of China (Nos. 20173064 and
90203017).
μ
Appendix A. Supplementary material
Supplementary data associated with this article can be
0
50
100
150
200
250
300
350
T / K
References
Fig. 4. Temperature-dependence of leff (h) and vÀm1 (s) for 1.
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along crystallographic c-axis in perfect face-to-face mode
with separation of 8.71 A. Although there are many
reported polymeric compounds with cobalt–carboxylate
chains [10], it is very rare that cobalt–carboxylate chains
array uniformly and evenly toward one direction in three-
dimensional polymeric network.
˚
Compound 1 exhibits shoulder peak (374 nm) and max-
imum peak (410 nm) in the emission spectrum. The first
emission peak is assigned to ILCT (intra-ligand charge-
transfer) excitation, because the similar emission peak
(370 nm) was also observed in emission spectrum of free
ligand H2DCNT. The second emission peak probably ori-
gins from LMCT (ligand-to-metal charge-transfer). One
nitrogen atom in the triazine ring coordinates to Co(II),
which favors charge-transfer from the donor group
diethylamino along aromatic triazine ring to Co(II).
The temperature-dependent magnetic susceptibility of 1
was measured in the 2–300 K region at 5KG applied field.
The leff and vÀm1 vs. T curves are shown in Fig. 4. The leff
value at 300 K is 5.26 B.M. which is larger than the uncou-
pling spin-only value of 3.87 B.M., indicating contribution
to the susceptibility from orbital angular momentum at
high temperature. The data in vÀm1 vs. T plots can be fitted
to the Curie–Weiss law, vm = Cm/(T À h), closely with
Cm = 3.76 cm3 K molÀ1 and h = À28.1 K. Upon cooling
to 2 K, the leff values decrease gradually to 1.69 B.M.
The drop of leff with T can be attributed largely to the sin-
gle-ion behavior of Co(II). These results indicate very weak
antiferromagnetic interactions between cobalt(II) centers,
which is consistent with crystal structure of compound 1,
where the exchange pathways between neighboring mag-
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[4] Diethylamine (3.66 g, 0.05 mol) in 20 ml acetone was added slowly
with stirring to a solution of cynanuric chloride (4.61 g, 0.025 mol) in
100 ml acetone at 0 °C, over a period of 45 min. The solution of p-
aminobenzoic acid (13.71 g, 0.1 mol) in 200 ml acetone was then
added, which created more white deposit. The mixture was heated to
45 °C and reacted with stirring for 12 h. After cooling, the white
product was filtered from the reaction mixture, washed free of
hydrochloric acid salt of diethylamine and p-aminobenzoic acid with
water, oven-dried at 60 °C in 76% yield. mp: 360–362 °C. Anal. Calc.
for H2DCNT Æ 2H2O: C 55.02, H 5.72, N 18.33, O 20.94. Found: C
55.13, H 5.75, N 18.24, O 20.86. 1H NMR (DMSO): N–H 10.128,
phen 7.902 7.781, H2O 3.650, –CH2 1.220, –CH3 1.194. IR (KBr
pellet, cmÀ1): 2974 b, 1687 s, 1631 s, 1583 s, 1549 s, 1421 m, 1313 s,
1288 m, 1258 s, 1171 s, 1091 w, 855 m, 769 m, 648 w.
[5] S.N.G. Acharya, R.S. Gopalan, G.U. Kulkarni, K. Venkatesan, S.
Bhattacharya, Chem. Commun. (2000) 1351.
˚
netic centers (CoÁ Á ÁCo distance: 4.69 A) involve l2-carbox-
ylate which actually serves as weak mediator of magnetic
exchange.
In summary, compound 1 represents a polymer based
upon the assembly of Co(II) and a new multifunctional
ligand H2DCNT and a rare case where infinite Co(II)
´
´
[6] J.-R. Galan-Mascaros, J.-M. Clemente-Juan, K.R. Dunbar, J. Chem.
Soc., Dalton Trans. (2002) 2710.