compared with those of ligand L1 as mentioned above. Such
differences in maximum emission and lifetime between complex
2 and L1 may probably be caused by Ag ؒ ؒ ؒ Ag interactions in
2, since no such interactions were found in 3 as revealed by
crystal structure analyses. It has been suggested that Ag ؒ ؒ ؒ Ag
interactions may have impact on the emissions.26
in complex 2 is very different from that in complex 3. In com-
plex 2, the silver() atoms have two types, namely, four- and two-
coordinate, while the complex 3 only contains four-coordinated
silver() atoms. The results are assigned to the different flexi-
bility of long chain ligands L1 and L2 and demonstrate the
important role of the nature of ligand on the assembly.
In the emission spectrum of complex 4 (Fig. 6c), a weak
photoluminescence with maximum emission at ca. 574 nm was
observed upon excitation at 250 nm. Similar photolumines-
cence has been reported for the 2D layered Cu() coordination
polymer with maximum emission at ca. 580 nm (ca. τ = 1.06 ns,
λex = 250 nm).27 The UV-vis spectrum of complex 4 exhibits a
low-energy band at ca. 402 nm in the solid state, which corre-
sponds to the metal-to-ligand charge transfer (MLCT).28 How-
ever, the metal center d to s orbital transition could not be
completely ruled out.27 It is well known that low-energy emis-
sions of [Cu(NN)2]ϩ (NN = 2,9-disubstituted-1,10-phenanthro-
line) systems are usually assigned to the metal-to-ligand d–π*
charge transfer (MLCT) and hence the observed luminescence
of 4 can be ascribed to the MLCT emission similar to the
reported Cu() complexes.29–31
During the past decades, the photoluminescence properties
of copper() complexes, especially with 2,9-disubstituted-1,10-
phenanthroline ligands, have been extensively examined.29 The
results showed that the emission behavior of these Cu() com-
plexes, e.g. emission wavelength, excited state lifetime, is quite
changeable depending on the chemical nature, size, and pos-
ition of substituents and distortions of the structure. To inhibit
the flattening distortion of the excited state, bulky substituents
in the ligands were introduced, and as a result, fluorescent
properties of their Cu() complexes were improved.29 On the
other hand, McMillin et al. reported the luminescent property
of a bis(phenanthroline)copper() complex without such steric
substituents in the solid state.31a The observation of this lumin-
escence is ascribed to the small flattening distortion probably
due to the packing interactions in the crystal, which prevent
further distortion in the photoexcited state. Compared with
these [Cu(NN)2]ϩ complexes, the coordination polymer 4, in
which the coordinated N atoms are of mixed types (two imino
Ns and two imidazole Ns), shows both flattening and rocking
distortions in the solid.32 The flattening distortion is demon-
strated by a dihedral angle of 98.7Њ between the planes defined
by Cu(1), N(1), N(2) and by Cu(1), N(12A), N(22B) (Fig. 4a),
and the rocking distortion is reflected by a long Cu(1)–N(2)
bond length [2.335(3) Å] compared with other three bonds
(Table 2) and an approximately pyramidal coordination geom-
etry around the copper() atom. Such distortions in the crystal
are probably induced by crystal packing interactions that
may also oppose further distortion in the excited state,31a and
as a consequence the coordination polymer 4 shows a weak,
short-lived emission (ca. τ = 1.7 ns) in the solid.
Acknowledgements
This work was supported by National Natural Science Found-
ation of China (Grant No. 20231020).
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Conclusion
The present study shows that the reactions of new long-chain
ligands L1 and L2 with various metal salts can afford a variety
of fascinating self-assembled polymeric frameworks. The dif-
ference between ligands L1 and L2 is that the former is more
flexible than the latter. Flexible ligand L1 can adjust its con-
formations to fit with the geometrical needs of transition metal
ions. In complex 1, ligand L1 adopts the compressed W-shape
to give a 2D rhombic grid network when it reacted with
cadmium() bromide. In the reaction with Ag() salt, long-chain
ligand L1 adopts conformations of U- and W-shapes to meet
the geometric need of four-coordinated and two-coordinated
Ag() atoms to form an infinite wandering 1D chain in complex
2 (Scheme 2). The relatively rigid ligand L2 only adopts a
U-shape conformation in complexes 3, 4 and 5 and its com-
plexes all exhibit an infinite zigzag 1D chain structures (Scheme
2). On the other hand, the coordination mode of silver() atoms
16 RDIF94: P. T. Beurskens, G. Admiraal, G. Beurskens, W. P. Bosman,
R. de Gelder, R. Israel and J. M. M. Smits, The DIRFID-94 program
system, Technical Report of the Crystallography Laboratory,
University of Nijmegen, The Netherlands, 1994.
D a l t o n T r a n s . , 2 0 0 3 , 1 8 3 6 – 1 8 4 5
1844