1·2. These results could be attributed to the extension of the
guests which place the N-methyl protons in different chemi-
cal environments compared with the complex 1·2. Moreover,
it was found that the complexes 1·3 and 1·4 also showed
slow rates of the complexation and decomplexation at room
temperature. Consequently, the association constants for the
the two pyridinium rings were well coplanar and parallel
with the anthracene rings of 1. These structural features of
complex 1·2 were quite different from those of the paraquat-
based complexes reported previously. We further found that
there existed not only two pairs of C-H···O hydrogen bonds
between the protons of N-methyl groups and the ether oxygen
atoms with the distances of 2.58 (a) and 2.64 Å (b),
respectively, but also a pair of face-face π-stacking interac-
tions between the pyridinium rings of the guest and the
aromatic rings of the host (dπ-π ) 3.37 Å for d). Moreover,
a pair of C-H· ··π interactions between the protons of
N-methyl groups and the aromatic rings of the host with the
distance of 2.80 Å (c) were also observed. These multiple
noncovalent interactions played an important role in forma-
tion of the stable complex, which is consistent with the result
in solution. Due to the planar skeleton and high symmetry
of the host in the complex, it was also found that by virtue
of three pairs of C-H···π interactions between the methylene
and methyl protons of host 1 and the adjacent anthracene
ring (dC-H· · ·π ) 2.62 for e, 2.75 for f, and 2.74 Å for h), and
a pair of C-H· ··O hydrogen bond between the methylene
proton and the ether oxygen atom of the host with the
distance of 2.65 Å (g), the complex 1·2 could self-assemble
into a linear supramolecular array, which further formed a
2D mosaic-like architecture12 (Figure 3b) by virtue of the
noncovalent interactions between the macrocycle and the
1:1 complexes 1·3 and 1·4 at Ka1·3 ) 1.4 × 106 and Ka·4
)
2.1 × 106 M-1, respectively, were obtained by the competi-
tive method.9
The electrospray ionization mass spectra (ESIMS) pro-
vided more evidence for formation of the stable 1:1
complexes 1·2, 1·3, and 1·4.9 Consequently, the strongest
- 2+
(base) peaks at m/z 679.7 for [1·2-2PF6 ] , 692.7 for [1·3-
- 2+
- 2+
2PF6 ] , and 717.9 for [1·4-2PF6 ] , respectively, were
observed.
Formation of the 1:1 complex between 1 and 2 was further
confirmed by its X-ray crystal structure.11 As shown in Figure
3a, it was found that the guest 2 was included in the central
solvent molecule and PF6 counterions.9
-
We also obtained single crystals of complexes 1·313 and
1·414 by diffusion of isopropyl ether into an equimolar
mixture of the host and the guest in CH3CN/CHCl3 (1:1,
v/v) solution. The crystal structures showed that the rodlike
guests 3 and 4 with considerable length (ca. 12.7 Å for 3
and 15.0 Å for 4) could also be completely included inside
the cavity of the host to form 1:1 complexes in the similar
complexation mode to the complex 1·2. As shown in Figure
4a,b, there existed multiple C-H· · ·O hydrogen bonding
(a ) 2.70, b ) 2.66, c ) 2.66, d ) 2.44, e ) 2.45, and f )
2.62 Å) between the N-methyl protons and the aromatic
proton of guest 3 and the ether oxygen atoms of the host
and also face-face π-stacking interactions between the
pyridinium rings of the guest and the aromatic rings of the
host with distances of 3.28 (g), 3.35 (h), 3.39 (i), and 3.34
Å (j), respectively. Moreover, it was found that complex 1·3
could also stack into a linear supramolecular array by
C-H· ··O hydrogen bonding (2.65 for A, and 2.60 Å for B),
and C-H· ··π interactions (2.78 for C, 2.62 for D, and 2.77
Å for E) between the two adjacent macrocycles, which
Figure 3. (a) Crystal structure of 1·2; the blue lines denote the
nocovalent interactions. (b) 2D mosaic-like sheet; the guests are
shown in blue. Solvent molecules, PF6- counterions, and hydrogen
atoms not involved in the interactions were omitted for clarity.
(12) (a) Ashton, P. R.; Claessens, C. G.; Hayes, W.; Menzer, S.; Stoddart,
J. F.; White, A. J. P.; Williams, D. J. Angew. Chem., Int. Ed. Engl. 1995,
34, 1862–1865. (b) Asakawa, M.; Ashton, P. R.; Brown, C. L.; Fyfe,
M. C. T.; Menzer, S.; Pasini, D.; Scheuer, C.; Spencer, N.; Stoddart, J. F.;
White, A. J. P.; Williams, D. J. Chem.sEur. J. 1997, 3, 1136–1150.
(13) Crystal data for 1·3·3CH3CN·CHCl3·H2O: C85H112F12N5O21P2; Mr
) 1936.09; triclinic, P1; a ) 10.5785(15) Å, b ) 12.5308(17) Å, c )
20.433(4) Å; R ) 97.683(11)°, ꢀ ) 97.630(11)°, γ ) 111.007(7)°; V )
2457.5(6) Å3; Z ) 1; d ) 1.308 g cm-3; T ) 173(2) K; R1 ) 0.1061, wR2
) 0.2293 (all data); R1 ) 0.0885, wR2 ) 0.2157 [I > 2σ(I)].
(14) Crystal data for 1·4·2CH3CN: C86H108F12N4O20P2; Mr ) 1807.70;
triclinic, P-1; a ) 11.732(2) Å, b ) 12.020(2) Å, c ) 18.224(3) Å; R )
79.289(5)°, ꢀ ) 85.127(6)°, γ ) 88.981(6); V ) 2516.1(8) Å3; Z ) 1; d )
1.193 g cm-3; T ) 173(2) K; R1 ) 0.0992, wR2 ) 0.2207 (all data); R1 )
0.0754, wR2 ) 0.2040 [I > 2σ(I)].
cavity of host 1 and the two N-methyl groups pointed to the
two dibenzo-30-crown-10 cavities, respectively. Moreover,
(11) Crystal data for 1·2·3CH3CN·2H2O: C82H111F12N5O22P2; Mr
)
1808.70; monoclinic, C2/c; a ) 28.597(6) Å, b ) 10.465(2) Å, c )
29.068(6) Å; ꢀ ) 95.36(3)°; V ) 8661(3) Å3; Z ) 4; d ) 1.387 g cm-3
;
T ) 173(2) K; R1 ) 0.0718, wR2 ) 0.1662 (all data); R1 ) 0.0650, wR2 )
0.1599 [I > 2σ(I)].
1890
Org. Lett., Vol. 12, No. 8, 2010