also reveals that the degrees of overlap between the TCNQ‚
‚‚TTF (containing C1 and C2) and TCNQ‚‚‚TTF (containing
C9 and C10) are not identical,18 indicating that the charge
transfer can be different for the two TTF parts in the same
molecule. In a TCNQ moiety, bond lengths tend to change
with an increase in the negative charge located on the
acceptor.
and substituted monopyrrolo-TTF25 (1.761(2) Å). 6‚TCNQ
exhibits a lower degree of intermolecular charge transfer than
TTF‚TCNQ,26 which is not surprising, since the oxidation
1
potential of 6 (E1/2 ) 0.37 V, vs Ag/AgCl in CH2Cl2) is
1
slightly higher than that of TTF (E1/2 ) 0.34 V, vs Ag/
AgCl in MeCN). The nitrile absorption frequency in the
solid-state IR spectrum of 6‚TCNQ is shifted to a lower
wavenumber27 (2195 cm-1) with respect to that of TCNQ
(2222 cm-1), which also suggests that a charge transfer
occurs between the TTF part and TCNQ in the solid state.28
In summary, a general and efficient method for the
preparation of TTF-belts has been developed. The TTF-belt
6 was designed to allow complexation of TCNQ inside its
cavity. However, a solid-state X-ray crystal structure analysis
of the CT complex 6‚TCNQ revealed that the TCNQ is
associated outside (alongside) one of the electron donors,
reflecting that the complicated and subtle balance between
all the individual noncovalent forces acting in cooperation
are difficult to predict. The efficient synthetic methodology
described in this letter allows us, in a few steps, to make
related TTF-belts in which the spacers can be varied in order
to optimize the complexation properties of the macrocyclic
host. Work is aimed in this direction, together with further
functionalization generating also TTF-cages incorporating
three or more monopyrrolo-TTF moieties.
It has been found that differences in the bond length of
TCNQ (Figure 5) change practically linearly19 from 0.069
Figure 5. Structure of TCNQ.
Å (b-c) and 0.062 Å (d-c) in neutral TCNQ20 to zero in
the TCNQ radical anion.21 In the case of 6‚TCNQ, the
average bond lengths are a ) 1.349(5) Å, b ) 1.433(4) Å,
c ) 1.389(4) Å, and d ) 1.426(5) Å, suggesting that the
charge transfer is ca. 0.4 e. A similar model of linearly
dependency22 can be applied for the central C-S bonds of
the TTF moiety, suggesting positive charges23 of 0.2 and
0.0 e, respectively, for the two TTFs in the same belt. This
inconsistency in balance between negative and positive
charges can presumably be ascribed to a change in central
C-S bond length between unsubstituted TTF24 (1.757(2) Å)
Acknowledgment. We thank University of Southern
Denmark for a Ph.D. Scholarship to K.N., Carlsbergfondet
for financial support to J.O.J., and Lars Duelund for recording
the EPR spectrum.
Supporting Information Available: Characterization
data for 3-6, together with crystallographic data for 6 and
6‚TCNQ. This material is available free of charge via the
(16) The crystal structure contains one solvent molecule per 6‚TCNQ,
and one of the spacer chains is somewhat disordered, which was modeled
by two slightly different conformations (only one of which is shown in
Figure 3).
(17) Deviations from planarity can be described by the interplanar angles
A-B 1.8°, A-C 3.5°, D-E 2.2°, and D-F 10.6° of 6‚TCNQ; translation
of the two TTF parts in the longitudinal direction was 4.5 Å.
(18) The overlap between TCNQ‚‚‚TTF (containing C9 and C10) is
largest.
OL025622Z
(25) The average bond length for the central C-S bonds in 6. If the
value 1.757 is changed to 1.761 Å in the equation described in ref 23, the
positive charges on the two TTF units are ca. 0.3 and ca. 0.1 e, respectively.
(26) Kistenmacher, T. J.; Phillips, T. E.; Cowan, D. O. Acta Cryst. 1974,
B30, 763-768.
(27) The change in absorption frequencies measured by IR spectroscopy
(2195 cm-1) suggests a charge transfer of ca. 0.7 e according to the model
proposed by Chappell and co-workers.28 However, these results are
inconsistent with the degree of charge transfer suggested by the crystal
structure analysis (ca. 0.4 e). A similar inconsistency has been observed in
CT complexes of BEDT-TTF‚TCNQ; see: Wu, W.; Zhang, D.; Li, H.;
Zhu, D. J. Mater. Chem. 1999, 9, 1245-1249.
(28) (a) Chappell, J. S.; Bloch, A. N.; Bryden, W. A.; Maxfield, M. O.;
Poehler, T.; Cowan, D. O. J. Am. Chem. Soc. 1981, 103, 2442-2443. (b)
Khatkale, M. S.; Devlin, J. P. J. Chem. Phys. 1979, 70, 1851-1859.
(19) Flandrois, S.; Chasseau, D. Acta Crystallogr., Sect. B 1977, 33,
2744-2750.
(20) Long, R. E.; Sparks, R. A.; Trueblood, K. N. Acta Crystallogr. 1965,
18, 932-939.
(21) Hoekstra, A.; Spoelder, T.; Vos, A. Acta Crystallogr., Sect. B 1972,
28, 14-25.
(22) Clemente, D. A.; Marzotto, A. J. Mater. Chem. 1996, 6, 941-946.
(23) The values 0.2 and 0.0 were determined from the equation f ) 1.757
Å - 0.0385(F+), where f is the average bond length of the central C-S
bonds in the CT complex, 1.757 Å is the average bond length of the central
C-S bonds in neutral unsubstituted TTF, and F+ is the degree of positive
charge on the TTF unit in the CT complex.
(24) Cooper, W. F. N.; Kenny, C.; Edmonds, J. W.; Nagel, A.; Wudl,
F.; Coppers, P. Chem. Commun. 1971, 889-890.
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Org. Lett., Vol. 4, No. 8, 2002