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0020919181
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Previous theoretical work on the thermolysis of vynilazides: (a) L. A. Burke, G. Leroy, M. Nguyen, and M. Sana, J. Am. Chem. Soc., 100, 3668 (1978); (b) H. R. Bock, R. Dammel, and S. Aygen, J. Am. Chem. Soc., 105, 7681 (1983); (c) T. Yamabe, M. Kaminoyama, T. Mintao, K. Hori, K. Isomura, and H. Taniguchi, Tetrahedron, 40, 2095 (1984); (d) L. I. Lohr, M. Hanamura, and K. Morokuma, J. Am. Chem. Soc., 105, 5541 (1983).
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0344943401
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0020805175
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Previous theoretical work on the thermolysis of vynilazides: (a) L. A. Burke, G. Leroy, M. Nguyen, and M. Sana, J. Am. Chem. Soc., 100, 3668 (1978); (b) H. R. Bock, R. Dammel, and S. Aygen, J. Am. Chem. Soc., 105, 7681 (1983); (c) T. Yamabe, M. Kaminoyama, T. Mintao, K. Hori, K. Isomura, and H. Taniguchi, Tetrahedron, 40, 2095 (1984); (d) L. I. Lohr, M. Hanamura, and K. Morokuma, J. Am. Chem. Soc., 105, 5541 (1983).
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85034287750
-
-
note
-
MP2/6-31G*, B3LYP/6-311 + G(3df,2p), and MP2/ 6-311G + (3df,2p) charge densities were also analyzed. We could not locate a ring critical point using the MP2/6-31G* charge density whereas the other two highest level charge densities produced almost coincident BCP properties and an identical topology compared with the B3LYP/6-31G* and QCISD/6-31G* analyses.
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-
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40
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85034299561
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note
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20 Thus, a (3, + 1) critical point [local depletion of ρ(r + (Combining right arrow above sign))] on the valence shell of the C3 atom, is found to be aligned with a (3, - 1) critical point [secondary local concentration of ρ(r + (Combining right arrow above sign))] on the valence shell of the N7 atom.
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-
-
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43
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85034300461
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note
-
c) - B)], where the A and B parameters were obtained by a least-square fitting procedure assigning n = 1 to methylamine, n = 2 to formaldimine, and n = 3 for hydrogen cyanide at the MP2/6-31G*; and B3LYP/6-31C* levels.
-
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-
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44
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0009780705
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(a) ∇H and ∇G ab initio values were computed using MP2(FC)/6-31G* frequencies and electronic energies approximated in an additive fashion as follows: E[QCISD(T)/ -311 + G(3df,2p)] ≈ E[QCISD(T)/6-31G*] + E[MP2/6-311 + (3df,2p)] - E[MP2/6-31G*]. See L. A. Curtiss, P. C. Redfem, B. J. Smith, and L. Radom, J. Chem. Phys., 104, 5148 (1996);
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Curtiss, L.A.1
Redfem, P.C.2
Smith, B.J.3
Radom, L.4
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45
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85034298551
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(b) ΔH and ΔG DFT values were computed using the B3LYP/6-31G* frequencies and B3LYP/6-311 + G(3df,2p)//B3LYP/6-31G* electronic energies
-
(b) ΔH and ΔG DFT values were computed using the B3LYP/6-31G* frequencies and B3LYP/6-311 + G(3df,2p)//B3LYP/6-31G* electronic energies.
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-
-
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46
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0011083273
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vib(T) were scaled using the recommended frequency scaling factors: A. P. Scott and L. Radom, J. Phys. Chem., 100, 16502 (1996).
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Scott, A.P.1
Radom, L.2
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47
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85034310034
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note
-
Although the results of the IRC calculations presented in Figure 2 could suggest some discontinuity near the TS, we checked that no HOMO-LUMO crossing takes place during the evolution of the system. A CISD/6-31G*//MP2/6-31G* single-point calculation at the TS also confirms that the singlet wave function is absolutely dominated by the HF reference wave function.
-
-
-
-
48
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85034309455
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note
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8 was located on the B3LYP/6-31G* PES. This intermediate is characterized by a C(ketene)-N(imine) bond distance of 1.608 Å and a notable charge transfer of 0.43 e from formaldimine to cyanoketene. However, only 0.6 kcal/mol at the B3LYP/6-31G* level is required to produce fragmentation of the zwitterion passing through the corresponding TS to yield the cyanoketene-formaldimine planar van der Waals cis-complex (0.5 kcal/mol more stable than the zwitterion). The inclusion of ZPVE provokes the disappearance of the zwitterionic intermediate on the PES given that the TS for fragmentation turns out to be 0.1 kcal/mol more stable than the zwitterion.
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