T. Gu et al. / Tetrahedron Letters 42 (2001) 2309–2312
2311
a
Table 1. Luminescence data in CH2Cl2
298 K
(ns)
77 K
b
b
umax (nm)
~
bem
umax (nm)
~
(ns)
1
2
436
428
1.0
1.0
0.61
0.81
425
412
1.0 (90%), 4.2 (10%)
1.2 (85%), 5.6 (15%)
a The fluorescence spectra and quantum yields were obtained upon excitation on the absorption maxima.
b uexc=337 nm, single photon counting apparatus.3b
layers. From these data, we can deduce a thickness of
,
66 A corresponding to approximately twice the length
of compound 1, and therefore to
a
bilayered
arrangement.
A conjugated derivative that assembles four OPV moi-
eties arising from a calix[4]arene core has been prepared
and we have shown that it can act as a rigid core for
the design of new p-conjugated liquid crystalline deriva-
tives. As well as the potential use of such a compound
in optoelectronic devices, the calix[4]OPV presented
here is a strongly luminescent receptor and, therefore, is
also potentially useful in the field of host–guest
chemistry.9,10
Figure 2. X-ray diffraction pattern of 1 recorded at 160°C.
Acknowledgements
cence of OPV’s in CH2Cl2 both at 298 K and in a rigid
77 K matrix (Table 1). The luminescence lifetimes at
room temperature are monoexponential (1.0 ns),
whereas at 77 K biexponential decays are recorded
(Table 1), probably as a consequence of the presence of
different ‘frozen’ rotameric forms in the solid matrix.3b
The luminescence spectra of 1 and 2 are qualitatively
similar; however, it is worth pointing out that the
fluorescence maxima of the calix[4]OPV is slightly red-
shifted and the emission quantum yield lower (Table 1).
The differences in the absorption and luminescence
properties of 1 and 2 seem to suggest that interchromo-
phoric interactions in the calix[4]OPVs take place.9
The authors would like to thank Dr. B. Heinrich for his
help with the X-ray measurements and L. Oswald for
technical assistance in the synthesis. T.G. thanks the
Direction de la Recherche of the French Ministry of
Research for a post-doctoral fellowship.
References
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The liquid crystalline properties of compound 1 have
been studied by differential scanning calorimetry
(DSC), X-ray diffraction and optical investigations.
Polarized optical microscopy observations revealed the
slow apparition of a fluid birefringent phase at 140°C
corresponding to the transition from an amorphous
solid into a liquid crystalline phase. The clearing point
was determined to be 180°C. Whereas the birefringent
optical texture was non-characteristic on cooling the
sample from the liquid isotropic phase, the X-ray dif-
fraction patterns recorded for 1 were typical of a smec-
tic type organization. As depicted in Fig. 2, the X-ray
diffraction pattern shows a diffuse band in the wide
,
angle region at ca. 4.5 A and five sharp diffraction
peaks (I–V) in the small angle region corresponding to
the spacing ratios 1:2:4:5:6. It is noteworthy that the
relative intensity of the even reflections when compared
with the odd ones was temperature dependent, indicat-
ing an evolution of the organization within adjacent