ferromagnetic ordering at lower temperatures in the order of few
millikelvin. Further work to confirm this behaviour is undergoing
together with new crystallisation tries in order to increase both
structural and magnetic dimensionalities.
This work has been supported by the EU under a Marie Curie
Research Training Network (contract ‘‘QuEMolNa’’ number
MRTN-CT-2003-504880) and by DGI (Spain) under project
MAT2003-04699.
Notes and references
{ Crystal data for a-PTMHC [(C25H6Cl9O12?6(C4H8O)]: trigonal, R-3,
˚
a 5 24.9133(6), b 5 24.9133(8), c 5 15.0874(8) A, a 5 b 5 90, c 5 120u,
3
Fig. 4 Magnetic characterization of solvates [PTMHC?(THF)6] (%) and
[PTMHC?(Et2O)3] (#) in the presence of their mother liquors. Product of
the magnetic susceptibility with the temperature as a function of the
temperature in the lower limit.
˚
˚
V 5 8109.7(5) A , Z 5 6, l(Mo–Ka) 5 0.71073 A, 13298 reflections
collected, 1761 independent reflections with I . 2s(I), R1 5 0.0678,
wR2 5 0.1884, GOF 5 1.044. Both kind of THF-molecule present
disorder. For C10–C13–O5, the disorder was not solved. For C14–C17–06
a 1 : 1 disorder model with partial overlying position (C15 5 C15A and
C17 5 C17A) and bond restraints was used. Hydrogen atoms of both
THF-molecules were neither found nor calculated. CCDC 276959. See
other electronic format.
˚
6.89A). Interdigitation of diethyl ether molecules, promoted by
3
…
˚
weak PTMHC–Et2O O1 H–Csp hydrogen bonds (2.71A, 166u),
belonging to neighbouring layers avoid interlayer chlorine–chlorine
short contacts and/or hydrogen bonding between PTMHC
molecules, leading to an ABC arrangement of the layers along
the c axis (Fig. 3c). As in the first THF solvate, crystallinity is
immediately lost when the crystals are removed from their mother
liquor.
§ Crystal data for b-PTMHC [(C25H6Cl9O12?3(C4H10O)]: trigonal, R-3,
˚
a 5 15.6488(8), b 5 15.6448(6), c 5 33.8402(7) A, a 5 b 5 90, c 5 120u,
3
˚
˚
V 5 7.1767(5) A , Z 5 6, l(Mo–Ka) 5 0.71073 A, 12097 reflections
collected, 1880 independent reflections with I . 2s (I), R1 5 0.0588,
wR2 5 0.1624, GOF 5 1.037. Data were measured on a Nonius
KappaCCD. Structure solutions were done using SHELXS86 and
10.1039/b508952b for crystallographic data in CIF or other electronic
format.
Variable temperature magnetic susceptibility data for as-
synthesized crystalline samples of both solvates were obtained on
a SQUID susceptometer, under a temperature range of 2–300 K,
in the presence of their mother liquors. In both cases, a
paramagnetic behavior was observed in the 20–300 K temperature
range, with x.T product values that fully agree with the
theoretically value of 0.375 emu.K.mol21, expected for uncorre-
lated spins (S 5 K) with g 5 2.0. Main differences were observed
below 20 K. For [PTMHC?(THF)6], the x.T value smoothly
1 (a) G. Desiraju, Crystal Engineering: The Crystal as a Supramolecular
Entity: Perspectives in Supramolecular Chemistry, Vol. 2, Wiley, New
York, 1996; (b) J. Bernstein, M. Etter and L. Leiserowitz, Structure
Correlation, Vol. 2, Chapt. 11, VCH, New York, 1994.
2 (a) J. Cirureda, M. Mas, E. Molins, F. Lanfranc de Panthou, J. Laugier,
J. Park, C. Paulsen, P. Rey, C. Rovira and J. Veciana, J. Chem. Soc.,
Chem. Commun., 1995, 709; (b) J. Cirujeda, E. Herna`ndez-Gasio´,
C. Rovira, J.-L. Stanger, P. Turek and J. Veciana, J. Mater. Chem.,
1995, 5, 243.
decreases upon decreasing temperature until
a value of
0.358 emu.K.mol21 at 2 K (Fig. 4)., consistenly with the presence
of very weak intermolecular antiferromagnetic interactions
(through space), in agreement with the lack of direct hydrogen
bonds between PTMHC radicals in that solvate. For
[PTMHC?(Et2O)3], the x.T value smoothly increases upon
decreasing temperature to reach a value of 0.395 emu.K.mol21
at 1.8 K (Fig. 4). This result is in agreement with the presence of
very weak intermolecular ferromagnetic interactions, which are
ascribed to the presence of direct hydrogen bonds between radical
molecules in this crystal structure.9
3 (a) K. Inoue and H. Iwamura, Chem. Phys. Lett., 1993, 207, 551; (b)
O. Fe´lix, M. W. Hosseini, A. De Cian, J. Fischer, L. Catala and
P. Turek, Tetrahedron Lett., 1999, 40, 2943; (c) C. Stroh, F. Romero,
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9, 875.
4 D. Maspoch, L. Catala, P. Gerbier, D. Ruiz-Molina, J. Vidal-Gancedo,
K. Wurst, C. Rovira and J. Veciana, Chem. Eur. J., 2002, 8, 3635.
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C. Rovira and J. Veciana, J. Am. Chem. Soc., 2004, 126, 730; (b)
D. Maspoch, N. Domingo, D. Ruiz-Molina, K. Wurst, G. Vaughan,
J. Tejada, C. Rovira and J. Veciana, Angew. Chem. Int. Ed., 2004, 43,
1828.
6 (a) S. Darlow, Acta Crystallogr., 1961, 14, 159; (b) J. Podlaha, I. Cisarova,
P. Holy and J. Zavada, Z. Kristallogr. - New Cryst. Struct., 1999, 214,
185; (c) J. Beeson, L. Fitzgerald, J. Gallucci, R. Gerkin, J. Rademacher
and A. Czarnick, J. Am. Chem. Soc., 1994, 116, 4621.
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Angew. Chem. Int. Ed., 1995, 34, 2654; (b) Q. Lin, S. Geib and
A. Hamilton, J. Chem. Soc., Perkin Trans. 2, 1998, 2109; (c) R. Kresinki
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50, 2039.
In summary, we have described the synthesis of a new PTM
radical derivative that is the first example of hexacarboxylic acid
with an electronic open-shell characteristic. Depending on the
solvent used, the self assembly of PTMHC molecules yield to
isolated radicals surrounded by THF molecules or to radical
hydrogen-bonded layers which are isolated by diethyl ether layers.
While weak antiferromagnetic interactions are obtained in the first
case, the presence of hydrogen bonds in the second one yields very
weak intermolecular ferromagnetic interactions in the solid state.
Taking into account the structural resemblance between the
[PTMHC?(Et2O)3] solvate and POROF-2,4b we can also expect a
8 A structure presenting comparable cell parameters and without disorder
for THF molecules has been obtained for compound 3 ([3?(THF)6]. See
Electronic Supplementary Information.
9 A similar behaviour was observed for crystalline a and b-phases of
PTMA. See Ref. 4.
This journal is ß The Royal Society of Chemistry 2005
Chem. Commun., 2005, 4801–4803 | 4803