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145
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0002259505
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For 6b and 6c, see: (b) Ashton, P. R.; Huff, J.; Menzer, S.; Parsons, I. W.; Preece, J. A.; Stoddart, J. F.; Tolley, M. S.; White, A. J. P.; Williams, D. J. Chem.-Eur. J. 1996, 2, 31-44.
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For 6b and 6c, see: (b) Ashton, P. R.; Huff, J.; Menzer, S.; Parsons, I. W.; Preece, J. A.; Stoddart, J. F.; Tolley, M. S.; White, A. J. P.; Williams, D. J. Chem.-Eur. J. 1996, 2, 31-44.
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146
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0035915382
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The monotosylates of 6a and 6b have been reported previously. See, respectively: (a) Collier, C. P.; Jeppesen, J. O.; Liu, Y.; Perkins, J.; Wong, E. W.; Heath, J. R.; Stoddart, J. F. J. Am. Chem. Soc. 2001, 123, 12632-12641.
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The monotosylates of 6a and 6b have been reported previously. See, respectively: (a) Collier, C. P.; Jeppesen, J. O.; Liu, Y.; Perkins, J.; Wong, E. W.; Heath, J. R.; Stoddart, J. F. J. Am. Chem. Soc. 2001, 123, 12632-12641.
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147
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(b) Liu, Y.; Saha, S.; Vignon, S. A.; Flood, A. H.; Stoddart, J. F. Synthesis 2005, 19, 3437-3445.
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For reviews of microwave-assisted reactions, see: (a) Kappe, O. C. Angew. Chem., Int. Ed. 2004, 43, 6250-6284.
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Lindstrom, P.1
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33744753747
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4+ ring and the diphenoxyterminated DNP polyemer, crystals of 1:1 and 3:1 complexes could be isolated. See: Northrop, B. H.; Khan, S. I.; Stoddart, J. F. Org. Lett. 2006, 8, 2159-2162.
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4+ ring and the diphenoxyterminated DNP polyemer, crystals of 1:1 and 3:1 complexes could be isolated. See: Northrop, B. H.; Khan, S. I.; Stoddart, J. F. Org. Lett. 2006, 8, 2159-2162.
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152
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33646722467
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6) are comparable to those observed in supramolecularly organized polymerizable diiodobutadiynes in the solid state: (a) Sun, A.; Lauher, J. W.; Goroff, N. S. Science 2006, 312, 1030-1034.
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6) are comparable to those observed in supramolecularly organized polymerizable diiodobutadiynes in the solid state: (a) Sun, A.; Lauher, J. W.; Goroff, N. S. Science 2006, 312, 1030-1034.
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153
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(b) Goroff, N. S.; Curtis, S. M.; Webb, J. A.; Fowler, F. W.; Lauher, J. W. Org. Lett. 2005, 7, 1891-1893.
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154
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The ∼45° tilt between the average planes of the π-donor and the π-acceptor rings in the catenanes 1b,c·4PF6 and 2b,c·4PF6 generates an element of helical chirality, such that molecules with (P) and (M) helicities can be identified. Additionally, 1,5-dioxynaphmalene and 1,2,3-triazole rings lose their symmetry elements once incorporated into a macrocycle. This desymmetrization imparts planar chirality of either a (pR) or a (pS) sense to both rings. Overall, these considerations mean that 1b,c·4PF6 can exist as a total of 23, 8 diastereisomers, while 2b,c·4PF6 could exist as a total of four diastereoisomers. X-ray crystallography, and 1H NMR spectroscopy reveal evidence for the existence of only one enantiomeric pair in the solid and solution states, respectively
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1H NMR spectroscopy reveal evidence for the existence of only one enantiomeric pair in the solid and solution states, respectively.
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155
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6 (Table 1) because of the geometry of the glycolic chain in the donor.
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6 (Table 1) because of the geometry of the glycolic chain in the donor.
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Alkyne units have been known to deform readily in strained systems, in extreme cases up to 52° over the four atoms of the X-C≡C-X unit. See, inter alia: (a) Eisler, S.; McDonald, R.; Loppnow, G. R.; Tykwinski, R. R. J. Am. Chem. Soc. 2000, 122, 6917-6928.
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Alkyne units have been known to deform readily in strained systems, in extreme cases up to 52° over the four atoms of the X-C≡C-X unit. See, inter alia: (a) Eisler, S.; McDonald, R.; Loppnow, G. R.; Tykwinski, R. R. J. Am. Chem. Soc. 2000, 122, 6917-6928.
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4+, DNP, and triazole peaks, consistent with the presence of only one (albeit unsymmetric) species.
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4+, DNP, and triazole peaks, consistent with the presence of only one (albeit unsymmetric) species.
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167
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4+-based [2]catenanes, see: (a) Vignon, S. A.; Stoddart, J. F. Collect. Czech. Chem. Commun. 2005, 70, 1493-1576.
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4+-based [2]catenanes, see: (a) Vignon, S. A.; Stoddart, J. F. Collect. Czech. Chem. Commun. 2005, 70, 1493-1576.
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168
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See also: b
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See also: (b) Tseng, H.-R.; Vignon, S. A.; Celestre, P. C.; Stoddart, J. F.; White, A. J. P.; Williams, D. J. Chem.-Eur. J. 2003, 9, 543-556.
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169
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This process is sometimes referred to as the pirouetting of the π-donating ring around the formally motionless CBPQT4+ ring. We prefer to treat this motion from a different system of reference as the circumrotation of the π-accepting ring around the formally motionless π-donating ring. This semantic distinction emphasizes the geometric equivalence of the above process with the circumrotation of the π-donating ring (rotation 3 in Figure 9, In both processes, one of the rings formally rotates around the axis going through its center, while the other ring remains motionless (and vice versa, Hence, the difference in the spectroscopic consequences of the two processes comes from the difference in the identity of the rotating ring, and not from different modes of rotation. See ref 44a as well as: (a) Ashton, P. R, Preece, J. A, Stoddart, J. F, Tolley, M. S, White, A. J. P, Williams, D. J. Synthesis 1994, 1344-1352
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4+ ring. We prefer to treat this motion from a different system of reference as the circumrotation of the π-accepting ring around the formally motionless π-donating ring. This semantic distinction emphasizes the geometric equivalence of the above process with the circumrotation of the π-donating ring (rotation 3 in Figure 9). In both processes, one of the rings formally rotates around the axis going through its center, while the other ring remains motionless (and vice versa). Hence, the difference in the spectroscopic consequences of the two processes comes from the difference in the identity of the rotating ring, and not from different modes of rotation. See ref 44a as well as: (a) Ashton, P. R.; Preece, J. A.; Stoddart, J. F.; Tolley, M. S.; White, A. J. P.; Williams, D. J. Synthesis 1994, 1344-1352.
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The circumrotation of the π-donating ring around the inner bipyridinum unit of the π-accepting ring brings about equilibration between two co-conformations. In a degenerate system, these co-conformations are of equal energy and thus are equally populated at any given point. The barriers for circumrotation in such systems are easily derived from the corresponding coalescence parameters. In nondegenerate systems, such as 1b, c·4PF6 and 2b,c·4PF6, two co-conformations are not of equal energy; accordingly, their populations and the relative intensities of 1H NMR signals are different. If the difference in population is sufficiently large >95:5, the circumrotation will be fundamentally unobservable by NMR spectroscopy since the only observable species will be the more stable co-conformation. This situation is spectroscopically indistinguishable from an alternative in which circumrotation does not occur at all. Although
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6 cannot be completely dismissed.
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(a) Liu, Y. et al. J. Am. Chem. Soc. 2005, 127, 9745-9759.
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Liu, Y.1
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