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19
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1842667821
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note
-
As we are focusing on the communication between the reaction and hydrogen-bonding centers, we will not elaborate on the numerous examples in which the hydrogen-bonding center coincides with the reaction center.
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21
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0004476581
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Westwood, J.6
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22
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J. D. Carr, S. J. Coles, M. B. Hursthouse, M. E. Light, J. H. R. Tucker, J. Westwood, Angew. Chem. 2000, 112, 3434-3437; Angew. Chem. Int. Ed. 2000, 39, 3296-3299.
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0035647892
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For recent reviews of ditopic receptors, see Ref.[11] and G. J. Kirkovits, J. A. Shriver, P. A. Gale, J. L. J. Sessler, J. Inclusion Phenom. Inclusion Phenom. Macrocycl. Chem. 2001, 41, 69-75.
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f) T. Tuntulani, S. Poompradub, P. Thavornyutikarn, N. Jaiboon, V. Ruangpornvisuti, N. Chaichit, Z. Asfari, J. Vicens, Tetrahedron Lett. 2001, 42, 5544.
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34
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33947483256
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-
See note 13 in ref. [7]. Briefly, the bond strengths of C-C, C-N, and N-N single bonds are not very different, but the bond strength of an N=N double bond is significantly weaker than those of C=N and C=C double bonds. Therefore it may be easier for the azo bridge to turn into form B in Scheme 2. Bond energies can be found in: S. W. Benson, J. Chem. Educ. 1965, 42, 502-518.
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Benson, S.W.1
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Adamo, C.23
Clifford, S.24
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Keith, T.44
Al-Laham, M.A.45
Peng, C.Y.46
Nanayakkara, A.47
Gonzalez, C.48
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Chen, W.52
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more..
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36
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84890021933
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S. F. Boys, F. Bernardi, Mol. Phys. 1970, 19, 553-566. Our BSSE calculation procedure is the same as in: L. Turi, J. J. Dannenberg, J. Phys. Chem. 1993, 97, 7899-7909.
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Mol. Phys.
, vol.19
, pp. 553-566
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Boys, S.F.1
Bernardi, F.2
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37
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33748602856
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S. F. Boys, F. Bernardi, Mol. Phys. 1970, 19, 553-566. Our BSSE calculation procedure is the same as in: L. Turi, J. J. Dannenberg, J. Phys. Chem. 1993, 97, 7899-7909.
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J Phys Chem.
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, pp. 7899-7909
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Turi, L.1
Dannenberg, J.J.2
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38
-
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1842768363
-
-
note
-
All reported energies are at the HF/6-31G* level. See the second paragraph of the Computational Details section for the reason for this choice of theory level.
-
-
-
-
39
-
-
1842717925
-
-
note
-
4-iminium.
-
-
-
-
40
-
-
1842667820
-
-
note
-
The values are the differences in the Mulliken group charge of pyrrole between protonated and neutral three-component systems.
-
-
-
-
41
-
-
41549096107
-
-
a values of the proton donors. For a recent example, see C. A. Holingsworth, P. G. Seybold, C. M. Hadad, Int. J. Quantum. Chem. 2002, 90, 1396-1403.
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Int. J. Quantum. Chem.
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-
-
Holingsworth, C.A.1
Seybold, P.G.2
Hadad, C.M.3
-
42
-
-
1842768364
-
-
note
-
2) of 0.9983 is obtained if the four deviating data points are not included in the correlation.
-
-
-
-
43
-
-
1842717926
-
-
note
-
H atoms were added (1.0 Å from the heavy atom along the original bond direction) to fulfill the valency requirement of pyrrole and the two-component system. In doing so, we avoided the spin-contamination problem of open-shell systems. This approximation appears to work well as evidenced by the reasonable results.
-
-
-
-
44
-
-
1842818700
-
-
note
-
LUMO and ΔE.
-
-
-
-
45
-
-
1842768365
-
-
note
-
n two-component systems.
-
-
-
-
46
-
-
1842768366
-
-
note
-
Since we want to illustrate a general phenomenon with Figure 4, we have used optimized geometries of closed-shell molecules, rather than the geometry found in the protonated three-component system.
-
-
-
-
47
-
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1842667822
-
-
note
-
4-H are reported.
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