ISMSC 2007 - Università degli Studi di Pavia
ISMSC 2007 - Università degli Studi di Pavia
ISMSC 2007 - Università degli Studi di Pavia
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Hierarchical self-assembly of <strong>di</strong>meric coor<strong>di</strong>nation cages<br />
Francesca Gruppi a , Marco Busi a , Enrico Dalcanale a<br />
a Dipartimento <strong>di</strong> Chimica Organica ed Industriale, <strong>Università</strong> <strong>di</strong> Parma, Viale G.P. Usberti 17/a,<br />
43100 Parma, Italy<br />
Metal-<strong>di</strong>rected self-assembly is a powerful tool for the construction of nanosize architectures<br />
performing specific functions. In previous works we have stu<strong>di</strong>ed the quantitative self-assembly<br />
of stable organopalla<strong>di</strong>um and organoplatinum coor<strong>di</strong>nation cages. [1, 2] The aim of the present<br />
work is the definition of hierarchical self-assembly protocols lea<strong>di</strong>ng to assembly of coor<strong>di</strong>nation<br />
cages networks. As a first step in this <strong>di</strong>rection, we have designed and synthesized tetradentate<br />
cavitand ligand 1, presenting three cyanophenyl and one ethynylpyri<strong>di</strong>ne ligands. The <strong>di</strong>fferent<br />
affinity of cavitand 1 ligands toward Pt(II) and Pd(II) complexes has been investigated. Among<br />
the several possibilities, the hierarchical self-assembly protocol of scheme 1 has been selected<br />
as the most valid approach to quantitative formation of a <strong>di</strong>meric coor<strong>di</strong>nation cage in solution.<br />
4<br />
4<br />
N N N<br />
O O<br />
O O O O O O<br />
R R R R<br />
6 Pd(dppp)OTf 2<br />
N<br />
O O<br />
Ph Ph Ph Ph<br />
NN N N<br />
P P<br />
N N<br />
NN<br />
PdL PdL<br />
PdL Pt<br />
Pt PdL PdLPdL<br />
NN N N<br />
O O<br />
Pt(tppb)OTf 2<br />
R R R R<br />
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R R R R<br />
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N N N N<br />
O OO O OO<br />
R R R R<br />
Ph<br />
P<br />
Ph<br />
OO<br />
N N N N<br />
R<br />
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N N<br />
OO O OOO OO<br />
R<br />
Pt<br />
Ph<br />
Ph<br />
P<br />
P<br />
R R<br />
R R<br />
Ph<br />
Ph<br />
R<br />
NN<br />
R<br />
Ph<br />
Ph<br />
P<br />
P<br />
Ph<br />
16<br />
Pt<br />
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OO<br />
[1] R. Pinalli, V. Cristini, V.Sottili, S. Geremia, M. Campagnolo, A. Caneschi, E. Dalcanale,<br />
J.Am. Chem.Soc., 2004, 126, 6516 – 6517<br />
[2] F. Fochi, P. Jacopozzi, E. Wegelius, K. Rissanen, P. Cozzini, E. Marastoni, E. Fisicaro, P.<br />
Manini, R. Fokkens, E. Dalcanale, J. Am. Chem. Soc., 2001,123, 7539 – 7552<br />
1<br />
R<br />
R R<br />
R R<br />
PSA 67<br />
R<br />
N<br />
N<br />
N N<br />
R<br />
PSA 68<br />
Circular Polarization of Fluorescence Emitted from a Supramolecular<br />
Complex of Achiral Conjugated Polymers and Neutral Polysaccharides<br />
S. Haraguchi 1 , M. Numata 1 , C. Li 1 , M. Fujiki 2 , K. Sakurai 3 and S. Shinkai 1<br />
1<br />
Department of Chemistry and Biochemistry, Graduate School of Engineering, Kyushu<br />
University, 744 Moto-oka, Nishi-ku, Fukuoka 819-0395, Japan<br />
2<br />
Graduate School of Materials Science, Nara Institute of Science and Technology, Takayama,<br />
Ikoma, Nara 630-0101, Japan<br />
3<br />
Department of Chemical Processes and Environments, Faculty of Environmental Engineering,<br />
The University of Kitakyushu, 1-1 Hibikino, Wakamatsu-ku, Kitakyushu, Fukuoka 808-0135,<br />
Japan -Conjugated polymers are nowadays used as the active layer in polymer light-emitting<br />
<strong>di</strong>odes (PLEDs). Several research groups have tried to control the linear polarization of the light<br />
output from the device by orienting the polymer chains in the film that are acting as the active<br />
layer. Hight degrees of linear polarization can be obtained in this way. As well as linearly<br />
polarized light sources, circularly polarized sources also find many applications in modern<br />
<strong>di</strong>splay technologies. In principle, it may be possible to construct a PLED that <strong>di</strong>rectly emits<br />
circularly polarized light by introducing molecular chirality into the conjugated polymer. Due to<br />
the break in the mirror-image symmetry, left or right circularly polarized light is then emitted and<br />
absorbed with <strong>di</strong>fferent probabilities. For example, by substituting poly(p-phenylene vinylene)<br />
with chiral side chains, PLEDs were indeed found to emit circularly polarized light. However, in<br />
such cases, <strong>di</strong>chroism (CD) and circularly polarized luminescence (CPL) in the -* transition<br />
region has generally been observed only when the polymer is in aggregated and solid film<br />
states, due to chiral supramacromolecular ordering resulting from intermolecular - stacking.<br />
For this reason the emission of the aggregated phase is weaker by 1 order of magnitude than<br />
that of the free chains. Therefore, the backbone helix structure, which does not depend on the<br />
aggregated phase, is believed to achieve a high quantum yield of circularly polarized<br />
luminescence. Recently, we demonstrated that supramolecular chiral insulated molecular wire<br />
can be formed between achiral water-soluble conjugated polymers and neutral polysaccharides<br />
(schizophyllan; SPG)(1). In the present work, we have focused on the use of this<br />
supramolecular chiral complex as a PLED that <strong>di</strong>rectly emits circularly polarized light.<br />
[1] C. Li, M. Numata, A. -H. Bae, K. Sakurai, S. Shinkai, J. Am. Chem. Soc., 127, 4548 (2005).