Table 1 Transition temperatures and thermodynamic dataa
Compound
Tonset/uC (DH/kJ mol21
)
L [Ref. 8]
L2m
L2e
Cr 79 (31.8) Cr’ 130 (13.1) SmC 180b SmA 183 (6.1) I
Cr 129 (59.7) I
Cr [122 (7.2) SmA]c 124 (56.1) I
Cr 108 (95.0) Cr’ 178 (53.2) I
[ZnL2Cl2]
[Zn(L2m)Cl2] Cr 97 (16.0) Cr’ 164 (27.2) I
[Zn(L2e)Cl2] Cr 95 (10.6) SmC 134 (13.7d ) SmA 154b
I
a Cr, Cr’: crystal phases, I: isotropic liquid, SmA: smectic A, SmC:
smectic C. b Optical microscopy data. c Monotropic transition.
d Transitions SmC–SmA and SmA–I appear by DSC as a single
peak.
Fig. 2 Absorption and emission spectra for compound L2e (dotted line) and
[Zn(L2e)Cl2] (solid line).
study new multifunctional materials based on zinc-containing
mesogens.
We thank the Diputacio´n General de Arago´n, the CICYT-
FEDER projects MAT2002-04118-CO2-02 and MAT2003-07806-
CO2-01, and the ‘‘Programa Ramo´n y Cajal’’ from the Ministerio
de Ciencia y Tecnolog´ıa (Spain) for financial support.
Notes and references
{ Crystal data for [Zn(bmpze)Cl2]: colourless crystals suitable for crystal-
lographic analysis were obtained by slow diffusion of hexane into a
solution of the compound in dichloromethane. C24H36Cl4N8Zn2, M ~
˚
709.15, monoclinic, a ~ 14.976(3), b ~ 11.164(3), c ~ 18.877(3) A, b ~
3
˚
101.590(9)u, V ~ 3091.8(10) A , T ~ 293 K, space group P21/c, Z ~ 4,
Fig. 1 (a) ORTEP representation of [Zn(bmpze)Cl2] (50% probability
ellipsoids) with atom numbering scheme. (b) Packing diagram showing two
kinds of planes parallel to bc.
m(Mo-Ka) ~ 1.926 mm21. The structure, refined on F2, converged for
5434 unique reflections (Rint ~ 0.0376) to give R1 ~ 0.0569, wR2 ~ 0.1270
[I w 2s(I)] and R1 ~ 0.1112, wR2 ~ 0.1536 (all data) and a goodness-of-
fit
achieve this goal proved unsuccessful. However, we were able to
solve the structure of [Zn(bmpze)Cl2] [bmpze: 1,2-bis(3,5-dimethyl-
pyrazolyl)ethane], in which the metal is in a similar environment,
and use this as a model for comparison.{ The molecular structure is
shown in Fig. 1a. The zinc atom is in a tetrahedral environment
and the planes containing the pyrazole rings are arranged with
respect to one another at an angle of only 16u, indicating that the
molecule is more planar than the ones with a methylene spacer.
From the packing study (Fig. 1b) it appears that the chloro ligands
are disposed in pseudoaxial and equatorial positions with respect to
the main molecular plane and the molecules are arranged in layers
in an antiparallel fashion.
b407652d/ for crystallographic data in .cif or other electronic format.
1 E. Kimura and T. Koike, Chem. Soc. Rev., 1998, 27, 179; H. Tanaka,
S. Tokito, Y. Taga and A. Okada, J. Mater. Chem., 1998, 8, 1999.
2 See for example Metallomesogens: Synthesis, properties and applications,
J. L. Serrano, ed., VCH, Weinheim, 1996.
3 B. A. Gregg, M. A. Fox and A. J. Bard, J. Chem. Soc., Chem. Commun.,
1987, 1134.
4 H. Adams, A. C. Albe´niz, N. A. Bailey, D. W. Bruce, A. S. Cherodian,
R. Dhillon, D. A. Dunmur, P. Espinet, J. L. Feijoo, E. Lalinde,
P. M. Maitlis, R. M. Richardson and G. Ungar, J. Mater. Chem., 1991,
1, 843.
5 E. Terazzi, J.-M. Benech, J.-P. Rivera, G. Bernardinelli, B. Donnio,
D. Guillon and C. Piguet, J. Chem. Soc., Dalton Trans., 2001, 769;
F. Morale, R. W. Date, D. Guillon, D. W. Bruce, R. L. Finn, C. Wilson,
A. J. Blake, M. Schro¨der and B. Donnio, Chem. Eur. J., 2003, 9, 2484.
6 G. Barberio, A. Crispini, M. Ghedini and D. Pucci, 8th International
Symposium on Metallomesogens, Book of abstracts O10, Namur,
Belgium, 2003.
7 W. Date, E. Fernandez Iglesias, K. E. Rowe, J. M. Elliott and
D. W. Bruce, Dalton Trans., 2003, 1914.
8 J. Barbera´, C. Cativiela, J. L. Serrano and M. M. Zurbano, Liq. Cryst.,
1992, 11, 887.
9 E. Diez-Barra, A. de la Hoz, A. Sa´nchez-Migallo´n and J. Tejeda,
Heterocycles, 1992, 34, 1365.
10 A. Lorenzotti, F. Bonati, A. Cingolani, D. Leonesi and C. Pettinari,
Gazz. Chim. Ital., 1991, 121, 551.
The mesophase assignment was confirmed by powder X-ray
diffraction14 at different temperatures. In the smectic C phase layer
˚
˚
spacings of 29 A (108 uC) and 30 A (118 uC) were measured. The
˚
smectic A phase was found to have a layer spacing of 32 A at
different temperatures (140, 145 and 150 uC). These values are in
accordance with a packing model similar to the mesophases of L
˚
˚
(measured layer spacing of 34.7 A in the SmA and 32–33 A for the
SmC)8 where the molecules are arranged with their long axes
perpendicular (SmA) or tilted (SmC) to the layer. It seems reason-
able that [Zn(L2e)Cl2] can lead to a smaller layer spacing as the
dimeric nature of the compound may leave more free volume to
accommodate the conformationally disordered decyloxy chains in
the layer.
11 E. Bouwman, W. L. Driessen, R. A. G. de Graaff and J. Reedijk, Acta
Crystallogr., Sect. C, 1984, 40, 1562.
12 B. Bovio, A. Cingolani and F. Bonati, Z. Anorg. Allg. Chem., 1992, 610,
151.
13 C. Pettinari, F. Marchetti, A. Cingolani, D. Leonesi, M. Colapietro and
S. Margadonna, Polyhedron, 1998, 17, 4145.
14 Powder XRD patterns were obtained using a pinhole camera (Anton-
Paar) operating with a point-focused Ni-filtered Cu-Ka beam and the
diffraction pattern was collected on flat photographic film. The samples
were held in Lindemann glass capillaries (1 mm diameter).
A preliminary study of the optical properties in dichloromethane
solutions showed that the ligand L2e exhibits fluorescence at 338 nm
upon excitation at the absorption maximum (263 nm). The zinc
complex [Zn(L2e)Cl2] fluoresces under similar conditions at 365 nm
with a higher intensity. Thus, on complexation both a red-shift and
a chelation-enhanced fluorescence, estimated to be multiplied by a
factor of three, are observed (Fig. 2).
Following this work we will apply the ‘‘flexible ligand’’ approach
to other structures in order to generate new phases as a way to
C h e m . C o m m u n . , 2 0 0 4 , 2 0 6 4 – 2 0 6 5
2 0 6 5