Angewandte
Chemie
[5] G. V. Oshovsky, D. N. Reinhoudt, W. Verboom, J. Am. Chem.
electron-deficient metallohost. This binding model was fully
supported by computer calculations (Figure 4)[20] and NMR
data: protons pointing inside the host were dramatically
shifted upfield (by more than 3 ppm for some of the inner
protons at the bridging positions, Table 1).
Soc. 2006, 128, 5270 – 5278.
[6] R. Pinalli, V. Cristini, V. Sottili, S. Geremia, M. Campagnolo, A.
Caneschi, E. Dalcanale, J. Am. Chem. Soc. 2004, 126, 6516 –
6517.
[7] Resorcinarene cavitands with o-phenylene derivatives at the
bridges result in cylindrical shapes: a) T. Heinz, D. M. Rudke-
vich, J. Rebek, Jr., Nature 1998, 394, 764 – 766; b) M. H. K.
Ebbing, M. J. Villa, J. M. Valpuesta, P. Prados, J. de Mendoza,
Proc. Natl. Acad. Sci. USA 2002, 99, 4962 – 4966; c) F. Hof, L.
Trembleau, E. C. Ullrich, J. Rebek, Jr., Angew. Chem. 2003, 115,
3258 – 3261; Angew. Chem. Int. Ed. 2003, 42, 3150 – 3153.
[8] E. Botana, K. Nattinen, K. Risannen, J. de Mendoza, Org. Lett.
2004, 6, 1091 – 1094.
[9] P. J. Stang, D. H. Cao, S. Saito, A. M. Arif, J. Am. Chem. Soc.
1995, 117, 6273 – 6283.
[10] M. L. Merlau, M. P. Mejia, S. T. Nguyen, J. T. Hupp, Angew.
Chem. 2001, 113, 4369– 4372; Angew. Chem. Int. Ed. 2001, 40,
4239– 4242.
[11] R. H. Vreekamp, W. Verboom, D. N. Reinhoudt, J. Org. Chem.
1996, 61, 4282 – 4288.
[12] a) T. J. Schwan, N. J. Miles, J. Heterocycl. Chem. 1982, 19, 1351 –
1353; b) E. W. Gill, A. W. Bracher, J. Heterocycl. Chem. 1983, 20,
1107 – 1109.
Figure 4. Top and side views of the optimized model of complex 12@
1·Re4. Receptor 1·Re4 is displayed in stick representation with a
transparent van der Waals radii surface except for the front wall (side
view). The octyl tails have been replaced by methyl groups for clarity.
Cavitand 12 is shown with a van der Waals radii surface.
[13] N. Margiotta, V. Bertolasi, F. Capitelli, L. Maresca, A. A. G. G.
Moliterni, F. Vizza, G. Natile, Inorg. Chim. Acta 2004, 357, 149–
158.
[14] J. L. Smithback, J. B. Helms, E. Schutte, M. Woessner, B. P.
Sullivan, Inorg. Chem. 2006, 45, 2163 – 2174.
[15] Up to six stereoisomers (oooo, oooi, ooii, oioi, iiio, and iiii; i =
inwards, o = outwards) can be predicted if it is assumed that the
bromine atom is always located in an apical position relative to
the plane containing the four metal centers.
[16] No such mixtures were reported for porphyrin squares, since the
stereoisomers averaged on the NMR time scale as a result of free
rotation of the pyridine ligands: R. V. Slone, J. T. Hupp, Inorg.
Chem. 1997, 36, 5422 – 5423.
[17] This was clearly seen in the NOESY spectrum (contacts between
the bulk water signal and the Ha and Hd cavitand signals).
[18] CCDC-618949 contains the supplementary crystallographic data
for this paper. These data can be obtained free of charge from
cam.ac.uk/data_request/cif.
Intermolecular NOE contacts observed between protons
Hb and Hc of the host and protons Hmeta and Hpara of guest 7, or
R1 (Me) protons of 12, also support the proposed geometry of
the complex (see Scheme 1 and Figure 3 for proton assign-
ment). Finally, the 7@1·Re4 inclusion complex was stable
enough to be detected by ESI-MS.
In summary, we have shown that a highly preorganized
metallocavitand 1·Re4 of nanoscopic dimensions can be
readily synthesized from a simple formyl-substituted calix[4]-
arene and 3,8-phenanthroquinone. Unsubstituted calix[4]ar-
enes and cavitands without substituents on the lower rim are
ideal guests for such a structure. Thus, for the first time, a
calixarene host becomes the guest. We are currently studying
an O-unsubstituted derivative of 1·Re4 that could self-
assemble into a continuous pile of bowl molecules. Also, the
use of the deep cavity of 1·Re4 for recognition and catalysis
studies is under active investigation.
[19] Single crystals were grown by slow evaporation of a CHCl3/
MeNO2 solution at RT. Data for 1·Re4 at 100 K:
C
129H135Br4N21O30Re4, 3524.02 gmolÀ1
¯
, triclinic, space group
Received: August 4, 2006
Published online: October 18, 2006
P1, a = 16.1122(19) , b = 23.443(3) , c = 23.654(3) , a =
113.546(3), b = 90.258(3), g = 99.928(3)8, V= 8041.1(16) 3,
Z = 2, 1calcd = 1.455 MgmÀ3, R1 = 0.1256 (0.2172), wR2 = 0.3259
(0.3960), for 20154 reflections with I > 2s(I) (for 40618 reflec-
tions (Rint: 0.0966) with a measured total number of 100297
Keywords: calixarenes · cavitands · N ligands · rhenium ·
.
supramolecular chemistry
reflections), GOF on F2 = 1.045, largest diff. peak (hole) = 6.628
À3
(À3.193) e
.
[20] CAChe WorkSystem Version 6.1.12.33. Fujitsu Limited.
[21] The deep calixarene 1 and the metallocavitand 1·Re4 are
luminescent, as are the formyl-substituted calixarenes 9 and
10, whereas the remaining calixarene and cavitand guests are
not. Addition of increasing amounts of guest to a solution of
1·Re4, keeping its concentration constant, caused an increase in
the intensity in the band at 550 nm.
[1] a) J. R. Moran, S. Karbach, D. J. Cram, J. Am. Chem. Soc. 1982,
104, 5826 – 5828; b) D. J. Cram, Science 1983, 219, 1177 – 1183.
[2] C. L. D. Gibb, E. D. Stevens, B. C. Gibb, J. Am. Chem. Soc. 2001,
123, 5849– 5850.
[3] E. S. Barret, J. L. Irwin, A. J. Edwards, M. S. Sherburn, J. Am.
Chem. Soc. 2004, 126, 16747 – 16749.
[4] L. R. MacGillivray, J. L. Atwood, Nature 1997, 389, 469– 472.
[22] SPECFIT, version 3.0.36, Spectrum Software Associates.
Angew. Chem. Int. Ed. 2007, 46, 198 –201
ꢀ 2007 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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