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46
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1842514642
-
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note
-
This value was also calculated at the same level in ref 3a.
-
-
-
-
47
-
-
1842619091
-
-
note
-
7′ (n = 1) was also optimized with both MP2/6-31G(d) and CASSCF-(10,10)/6-31G(d). In both cases, delocalized structures resulted that are extremely similar to that found with B3LYP/6-31G(d) (see Figure 1).
-
-
-
-
48
-
-
1842619092
-
-
note
-
For two similarly tethered infinite polyacetylene chains, a second set of orbitals is also present, with coefficients on the other carbons of the polyene chains. The nature of the linking framework would keep these carbons quite a bit farther apart than the bridgehead carbons, however, leading to only very small through-space interactions and a pair of nearly degenerate orbitals at the orbital frontier. It is possible, therefore, that the infinite system might have a triplet ground state, albeit of a rather different nature than the oligomers we study.
-
-
-
-
49
-
-
0345135031
-
-
One system with fused semibullvalene units was also examined (selected distances shown in Å): (diagram presented) This molecule is a highly strained (note in particular the 134° angle at the central carbon) and curved molecule (now with a direction of curvature opposite that of 8), but still contains close interpolyene contacts. This molecule can also be considered a member of the class of molecules known as fenestranes: molecules containing a central quaternary carbon that serves as a corner for four fused rings that are arrayed like the panes of a window or the "four comers" states of the American southwest. For leading references on fenestranes, see: (a) Georgian, V.; Saltzman, M. Tetrahedron Lett. 1972, 4315-4317.
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Georgian, V.1
Saltzman, M.2
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50
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0001187285
-
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(b) Thommen, M.; Keese, R. Synlett 1997, 231, and references therein. It should be noted that a structure with a localized inter-polyene single bond at one end is slightly more stable than this structure (by ∼2 kcal/mol, based on electronic energies).
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Synlett
, pp. 231
-
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Thommen, M.1
Keese, R.2
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51
-
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1842462370
-
-
A "side view" of structure 23: (diagram presented)
-
A "side view" of structure 23: (diagram presented)
-
-
-
-
52
-
-
0035913750
-
-
We have not yet studied the seemingly less constrained way to hold two polyenes in proximity to each other that has been explored by W. von. E. Doering and co-workers and Hopf and co-workers (Doering, W. von E.; He, J.; Shao, L. J. Am. Chem. Soc. 2001, 123, 9153-9151; Schüll, V.; Hopf, H. Tetrahedron Lett. 1981, 22, 3439-3442), who examined derivatives of bis-polyenyl cyclobutanes: (diagram presented)
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Doering, W.V.E.1
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53
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0003100791
-
-
We have not yet studied the seemingly less constrained way to hold two polyenes in proximity to each other that has been explored by W. von. E. Doering and co-workers and Hopf and co-workers (Doering, W. von E.; He, J.; Shao, L. J. Am. Chem. Soc. 2001, 123, 9153-9151; Schüll, V.; Hopf, H. Tetrahedron Lett. 1981, 22, 3439-3442), who examined derivatives of bis-polyenyl cyclobutanes: (diagram presented)
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Tetrahedron Lett.
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Schüll, V.1
Hopf, H.2
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54
-
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0032517378
-
-
and ref 19
-
σ-Bond cleavage in certain polyenes to produce two polyenyl radicals has been shown previously to be facile. See, for example: Beno, B. R.; Fennen, J.; Houk, K. N.; Lindner, H. J.; Hafner, K. J. Am. Chem. Soc. 1998, 120, 10490-10493, and ref 19.
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55
-
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1842514643
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note
-
CASSCF(14,14)/6-31G(d) and CASPT2/6-31G(d) single-point calculations agree that the fully delocalized 7' (n = 2) is more stable than the end-closed form (by ∼-1 kcal/mol with CASSCF and by ∼-6 kcal/mol with CASPT2).
-
-
-
-
56
-
-
1842619093
-
-
note
-
B3LYP was also previously shown to give energy differences for 7 and 7′ (n = 0, barbaralane) that were quite similar to those computed with CASPT2. See ref 3c.
-
-
-
-
57
-
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1842462371
-
-
note
-
Structures for 7′ (n = 1) with localized terminal inter-polyene bonds were also explored using the B3LYP/6-31G(d)//B3LYP/6-31G(d), CASSCF-(10,10)/6-31G(d)//B 3LYP/6-31G(d), CASPT2/6-31G(d)//B3LYP/6-31G(d), CASSCF(10,10)/6-31 G(d)//CASSCF(10,10)/6-31G(d), and CASPT2/6-31G-(d)//CASSCF(10, 10)/6-31G(d) levels. The results are shown in Table 5. B3LYP and CASPT2 energy calculations agree that the end-closed and open (fully delocalized) structures are very similar in energy-irrespective of the method used for the geometry optimization-while CASSCF consistently predicts that the end-closed form is considerably more stable than the open form (by 5-6 kcal/mol). Generally, CASPT2 energy calculations are considered to be more reliable than CASSCF energy calculations, and B3LYP has been shown to give similar results to CASPT2 for various reactions.
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Frölich, W.; Dewey, H. J.; Deger, H.; Dick, B.; Klingensmith, K. A. ; Püttmann, W.; Vogel, E.; Hohlneicher, G.; Michl, J. J. Am. Chem. Soc. 1983, 105, 6211-6220. The presence of "weak transannular interactions" has been suggested for these molecules.
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Frölich, W.1
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Püttmann, W.6
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Michl, J.9
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(b) Gunther, H.; Schmickler, H.; Brinker, U. H.; Nachtkamp, K.; Wassen, J.; Vogel, E. Angew. Chem. 1973, 85, 762-763, and references therein.
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Vogel, E.6
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68
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Application of the NICS technique to the polyacenes is described in: Schleyer, P. v. R.; Manoharan, M.; Jiao, H.; Stahl, F. Org. Lett. 2001, 3, 3643-3646. For a related study, see: Poater, J.; Fradera, X.; Duran, M.; Solà M. Chem. Eur. J. 2003, 9, 1113-1122.
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Schleyer, P.V.R.1
Manoharan, M.2
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69
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Application of the NICS technique to the polyacenes is described in: Schleyer, P. v. R.; Manoharan, M.; Jiao, H.; Stahl, F. Org. Lett. 2001, 3, 3643-3646. For a related study, see: Poater, J.; Fradera, X.; Duran, M.; Solà M. Chem. Eur. J. 2003, 9, 1113-1122.
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Poater, J.1
Fradera, X.2
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Solà, M.4
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70
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1842566979
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note
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The NICS values in Figure 5 were computed at the GIAO-B3LYP/6-31G-(d) level. These are similar to (and consistently ∼-1 ppm more negative than) those computed previously at the IGLO/DZ2P//B3LYP/6-311+G** level: -9.7 for benzene, -8.9 for naphthalene, -7.6 and -11.5 for anthracene, and -6.6 and -11.4 for tetracene.
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