Scheme 2 The number in parenthesis indicates the transition enthalpy; X is
a highly ordered mesophase and yet to be fully characterized; K
crystal.
=
entities connected by flexible spacers. The compound is
multifunctional, containing themochromic and photochromic
mesogenic units. Such substances have potential as materials
for information storage technology and replace mixtures of
mesogenic compound in different applications, thereby solving
phase separation problems associated with such mixtures. These
may perhaps also serve as model compounds (which are yet to
be realized) for co-polymeric liquid crystals. Interestingly, this
oligomer stabilizes a recently discovered UTGCC* phase—
supposed to be a highly frustrated phase—over a wide
temperature range of 90 °C and thus invites systematic
investigations so as to understand this behavior.
We are grateful to Professor S. Chandrasekhar for many
useful discussions and thankfully acknowledge Dr Geeta G.Nair
for her help in the experiments.
Notes and references
† The trimesogen CII-105 and other intermediates exhibited spectral data
consistent with their molecular structure. Selected data for CII-105:
nmax(KBr)/cm21 2950, 2863, 1729, 1607 and 1578; dH(500 MHz, CDCl3)
7.89 (d, J 8.9, 2H, Ar), 7.8 (d, J 8.15, 2H, Ar), 7.44 (d, J 5.9, 2H, Ar), 7.42
(d, J 5.8, 2H, Ar), 7.3 (d, J 8.15, 2H, Ar), 7.0 (d, J 8.95, 2H, Ar), 6.87 (d,
J 8.75, 2H, Ar), 6.84 (d, J 8.85, 2H, Ar), 5.36 (br d, J 4.85, 1H, olefinic), 4.6
(m, 1H, CHOCO), 4.12 (br t, 2H, OCH2), 4.06 (br t, 2H, OCH2), 3.96 (t, J
6.4, 2H, OCH2), 2.68 (t, J 7.65, 2H, ArCH2), 2.31 (m, 4H, 2 3 CNCH2),
2.01–0.9 (m, 40H, 17 3 CH2, 6 3 CH), 1.02 (s, 3H, CH3), 0.94 (t, J 7.25,
3H, CH3), 0.91 (d, J 6.5, 3H, CH3), 0.87 (d, J 2.1, 3H, CH3), 0.86 (d, J 2.1,
3H, CH3) and 0.67 (s, 3H, CH3); dC(100 MHz, CDCl3) 172.93, 161.22,
158.87, 158.75, 151.05, 147.1, 145.73, 139.67, 132.83, 128.99, 124.54,
122.59, 122.51, 115.8, 115.61, 114.67, 114.5, 88.04, 87.91, 73.82, 67.77,
67.69, 67.48, 56.69, 56.16. 50.05, 42.31, 39.74, 39.51, 38.16, 36.99, 36.59,
36.19, 35.77, 35.52, 34.54, 33.41, 31.88, 28.87, 28.2, 27.82, 25.95, 25.57,
24.76, 24.26, 23.83, 22.77, 22.53, 22.3, 21.03, 19.28, 18.71, 13.88 and
11.835; m/z (FAB) 1001 [MH]+ (calc. for C67H88N2O5).
Fig. 1 Optical microscopic texture observed (magnification 4003) for the
UTGBC* phase at 212.3 °C while cooling from the N* phase. (a) The
Grandjean Cano lines (the two striations running from the top to the bottom
of the picture) indicate the presence of a helix whose axis is normal to the
photograph.The square grid patterns [shown on an enlarged scale in (b)]
arise from a two-dimensional modulation perpendicular to the helix. The
simultaneous existence of both these features is supposed to be proof of the
existence of the UTGCC* phase.
periodicity is approximately the same as that of the spacing in
the square grid pattern mentioned above. Again, the filament
texture remains unchanged down to 119 °C. The features
described here for the low temperature mesophase are identical
to the textural observations for the very recently reported10
undulated twist grain boundary (UTGBC*) phase in a binary
system as well as in a single compound. While in the binary
mixture the UTGBC* phase is reported to occur over a narrow
range of temperature ( ~ 4 °C),10a the range is not mentioned in
the case of the single compound.10c In view of these
observations it is remarkable that the second mesophase in CII-
105, which shows the essential features of the UTGBC* phase,
viz. simultaneous existence of a square grid texture and a helical
structure perpendicular to it, exists over a large temperature
range of 90 °C. According to the proposed model,10a the
UTGBC* phase is a highly frustrated phase characterized by
modulations in all the three dimensions, with the two-
dimensional undulation of the smectic C*-like blocks being
orthogonal to the helix of the TGB structure. Hence, it is all the
more interesting to see that a phase with such a highly-frustrated
structure exists over a wide temperature range. The mesophase
below 119 °C seems to be a highly ordered one, and its detailed
characterisation is underway.
1 For a brief but recent review on dimers and oligomers see: C. T. Imrie
and G. R. Luckhurst, HandBook of Liquid Crystals, ed. D. Demus, J.
Goodby, G. W. Gray, H.-W. Spiess and V. Vill, Wiley-VCH,
Weinheim, 1998, vol. 2B, p. 801.
2 A. C. Griffin and T. R. Britt, J. Am. Chem. Soc., 1981, 103, 4957;
J. C. W. Chien, R. Zhou and C. P. Lillya, Macromolecules, 1987, 20,
2340.
3 (a) C. T. Imrie, F. E. Karasz and G. S. Attard, Macromolecules, 1993,
26, 545; (b) C. T. Imrie, F. E. Karasz and G. S. Attard, Macromolecules,
1993, 26, 3803.
4 J.-I. Jin, H.-S. Kim, J.-W. Shin, B. Y. Chung and B.-W. Jo, Bull. Korean
Chem. Soc., 1990, 11, 209; F. Hardouin, M. F. Achard, J.-I. Jin, J.-W.
Shin and Y.-K. Yun, J. Phys. II, 1994, 4, 627; C. V. Yelamaggad, A.
Srikrishna, D. S. Shankar Rao and S. Krishna Prasad, Liq. Cryst., 1999,
26, 1545.
5 (a) C. V. Yelamaggad, Mol. Cryst. Liq. Cryst., 1998, 326, 149; (b) C. V.
Yelamaggad, D. S. Shankar Rao and S. Krishna Prasad, unpublished
work.
6 G. S. Attard and C. T. Imrie, Liq. Cryst., 1989, 6, 387; R. Centore, A.
Roviello and A. Sirigu, Mol. Cryst. Liq. Cryst., 1990, 182B, 233; T.
Ikeda, T. Miyamoto, S. Kurihara, M. Tsukada and S. Tazuke, Mol.
Cryst. Liq. Cryst., 1990, 182B, 357; A. T. M. Marcelis, A. Koudijs and
E. J. R. Sudholter, Liq. Cryst., 1995, 18, 851; A. T. M. Marcelis, A.
Koudijs and E. J. R. Sudholter, Liq. Cryst., 1996, 21, 87; J. Andersch, S.
Diele, D. Lose and C. Tschierske, Liq. Cryst., 1996, 21, 103.
7 H. Furuya, K. Asahi and A. Abe, Polym. J., 1986, 18, 779.
8 S. H. Chen, D. Katsis, A. W. Schmid, J. C. Mastrangelo, T. Tsutsui and
T. N. Blanton, Nature, 1999, 397, 506; D. J. Broer, J. Lub and G. N.
Mol, Nature, 1995, 378, 467; E. Sackmann, J. Am. Chem. Soc., 1971,
93, 7088.
The transition temperatures obtained from the cooling mode
DSC scan along with the enthalpies are given in Scheme 2 (the
transition from the cholesteric to the second mesophase was too
weak for any reliable calculation of the enthalpy). It is worth
mentioning here that the trimesogen CII-105 is thermally stable
during repeated heating and cooling cycles through the
1
mesophases–isotropic transition, as confirmed by a H NMR
9 G. Attard and G. Williams, Nature, 1987, 326, 544.
10 (a) P. A. Pramod, R. Pratibha and N. V. Madhusudhana, Curr. Sci.,
1997, 73, 761; (b) G. G. Nair, Curr. Sci., 1998, 74, 98; (c) B. K.
Sadashiva, Pramana, 1999, 53, 213.
scan of the same sample which had been subjected to the DSC
experiments. The profile obtained was identical, within experi-
mental error, to that for the pristine sample.
In conclusion we have achieved the synthesis of the first
trimesogen containing three non-identical calamitic mesogenic
Communication a907974b
58
Chem. Commun., 2000, 57–58