Communications
lene protons, located ortho and meta to the amide nitrogen
such as linear polymerizations, with the product extending out
of the host cavity as it forms.
atom. Because of the orientation of the naphthyl ring, the
para proton is directed away from the alkyl chain and strong
cross peaks are not observed with the guest. Relative
distances between the host and guest protons in the
[RuC6ꢀGa4L6]12À system were determined from NOE inter-
action growth rates and show these two protons are the closest
to the protruding alkyl chain on the C3-related edges of the
three naphthalene rings that surround the aperture. These
hydrogen atoms are directed away from the cluster center and
can be used as boundary markers to distinguish the host
interior from the exterior. Methylene groups 4 and 5 are
closest to the boundary, whereas methylene group 1 is the
farthest. This difference suggests that the two naphthyl
protons are situated between the C4 and C5 of the alkyl
chain, with C4 on the interior side and C5 on the exterior side
of the cavity boundary. C1, immediately adjacent to the
encapsulated cationic head group, lies deep within the cluster.
Future NOE interaction growth studies will address the
specific conformations of the alkyl chain for guests with
different chain lengths.
Received: June 23, 2005
Published online: November 22, 2005
Keywords: host–guest systems · sandwich complexes ·
.
supramolecular chemistry · zwitterions
[1] D. S. Lawrence, T. Jiang, M. Levett, Chem. Rev. 1995, 95, 2229.
[2] S. Leininger, B. Olenyuk, P. J. Stang, Chem. Rev. 2000, 100, 853.
[3] M. M. Conn, J. Rebek, Jr., Chem. Rev. 1997, 97, 1647.
[4] M. A. Manteos-Timoneda, M. Crego-Calama, D. N. Reinhoudt,
Chem. Soc. Rev. 2004, 33, 363.
[5] T. D. Hamilton, L. R. MacGillvray, Cryst. Growth Des. 2004, 4,
419.
[6] M. Yoshizawa, Y. Takeyama, T. Kusukawa, M. Fujita, Angew.
Chem. 2002, 114, 1403; Angew. Chem. Int. Ed. 2002, 41, 1347.
[7] M. Fujita, M. Tominaga, A. Hori, B. Therrien, Acc. Chem. Res.
2005, 38, 371.
[8] V. F. Slagt, J. N. H. Reek, P. C. J. Kamer, P. W. N. M. van Leeu-
wen, Angew. Chem. 2001, 113, 4401; Angew. Chem. Int. Ed. 2001,
40, 4271.
[9] V. F. Slagt, P. W. N. M. van Leeuwen, J. N. H. Reek, Angew.
Chem. 2003, 115, 5777; Angew. Chem. Int. Ed. 2003, 42, 5619.
[10] V. F. Slagt, P. C. J. Kamer, P. W. N. M. van Leeuwen, J. N. H.
Reek, J. Am. Chem. Soc. 2004, 126, 1526.
High-resolution negative ion electrospray mass spectrom-
etry (ESI MS) confirmed the formation of host–guest com-
plexes (Figure 6). Spectra were obtained for solutions of the
[11] F. Hof, S. L. Craig, C. Nuckolls, J. Rebek, Jr., Angew. Chem.
2002, 114, 1556; Angew. Chem. Int. Ed. 2002, 41, 1488.
[12] J. M. Kang, J. Rebek, Jr., Nature 1997, 385, 50.
[13] J. M. Kang, J. Santamaria, G. Hilmersson, J. Rebek, Jr., J. Am.
Chem. Soc. 1998, 120, 3650.
[14] J. M. Kang, J. Santamaria, G. Hilmersson, J. Rebek, Jr., J. Am.
Chem. Soc. 1998, 120, 7389.
[15] A. J. Terpin, M. Ziegler, D. W. Johnson, K. N. Raymond, Angew.
Chem. 2001, 113, 161; Angew. Chem. Int. Ed. 2001, 40, 157.
[16] D. L. Caulder, R. E. Powers, T. N. Parak, K. N. Raymond,
Angew. Chem. 1998, 110, 1940; Angew. Chem. Int. Ed. 1998,
37, 1840.
[17] M. Ziegler, J. J. Miranda, U. N. Andersen, D. W. Johnson, J. A.
Leary, K. N. Raymond, Angew. Chem. 2001, 113, 755; Angew.
Chem. Int. Ed. 2001, 40, 733.
[18] D. L. Caulder, C. Bruckner, R. E. Powers, S. Konig, T. N. Parak,
J. A. Leary, K. N. Raymond, J. Am. Chem. Soc. 2001, 123, 8923.
[19] M. Ziegler, A. V. Davis, D. W. Johnson, K. N. Raymond, Angew.
Chem. 2003, 115, 689; Angew. Chem. Int. Ed. 2003, 42, 665.
[20] T. N. Parak, D. L. Caulder, K. N. Raymond, J. Am. Chem. Soc.
1998, 120, 8003.
Figure 6. Portion of the electrospray mass spectrum of the
[RuC10ꢀGa4L6]12À system that shows two adjacent peaks for the z=À4
charge state, with predicted isotopic distribution patterns for two particular
fragment ion formulae.
[21] T. N. Parac, M. Scherer, K. N. Raymond, Angew. Chem. 2000,
112, 1288; Angew. Chem. Int. Ed. 2000, 39, 1239.
[RuC4ꢀGa4L6]12À, [RuC6ꢀGa4L6]12À, [RuC8ꢀGa4L6]12À, and
[RuC10ꢀGa4L6]12À systems, and the resulting spectra showed
peaks for the z = À3 and À4 charge states of the host–guest
complexes with K+, Na+, and/or H+ counterions. The mass
spectra of the [RuC4ꢀGa4L6]12À and [RuC10ꢀGa4L6]12À sys-
tems show additional peaks that correspond to the z = À5
charge state of the host–guest complex.
[22] M. Ziegler, J. L. Brumaghim, K. N. Raymond, Angew. Chem.
2000, 112, 4285; Angew. Chem. Int. Ed. 2000, 39, 4119.
[23] D. H. Leung, D. Fiedler, R. G. Bergman, K. N. Raymond,
Angew. Chem. 2004, 116, 981; Angew. Chem. Int. Ed. 2004, 43,
963.
[24] D. Fiedler, R. G. Bergman, K. N. Raymond, Angew. Chem. 2004,
116, 6916; Angew. Chem. Int. Ed. 2004, 43, 6748.
[25] D. Fiedler, D. H. Leung, R. G. Bergman, K. N. Raymond, Acc.
Chem. Res. 2005, 38, 351.
[26] A. V. Davis, K. N. Raymond, J. Am. Chem. Soc. 2005, 127, 7912.
[27] L. Trembleau, J. Rebek, Jr., Science 2003, 301, 1219.
[28] D. Fiedler, D. Pagliero, J. L. Brumaghim, R. G. Bergman, K. N.
Raymond, Inorg. Chem. 2004, 43, 846.
This study shows that the [Ga4L6]12À tetrahedron remains
intact upon incorporation of the cationic head of a zwitterion,
while the link to the anionic tail passes through one of the
small openings at the centers of the triangular faces. This
process is fully consistent with the nondissociative guest-
exchange mechanism recently described.[26] If a guest can
extend out of the cavity, new reactions may be envisioned,
86
ꢀ 2006 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2006, 45, 83 –86