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1
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84899804555
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For selected reviews on developing quantitative theoretic descriptors of reactivities, see:
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For selected reviews on developing quantitative theoretic descriptors of reactivities, see:
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2
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0038661201
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P. Geerlings, F. DeProft, W. Langenaeker, Chem. Rev. 2003, 103, 1793-1874;
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Geerlings, P.1
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H. Mayr, M. Patz, Angew. Chem. 1994, 106, 990; Angew. Chem. Int. Ed. Engl. 1994, 33, 938;
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Mayr, H.1
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13
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0035802329
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H. Mayr, T. Bug, M. F. Gotta, N. Hering, B. Irrgang, B. Janker, B. Kempf, R. Loos, A. R. Ofial, G. Remennikov, H. Schimmel, J. Am. Chem. Soc. 2001, 123, 9500;
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Mayr, H.1
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Hering, N.4
Irrgang, B.5
Janker, B.6
Kempf, B.7
Loos, R.8
Ofial, A.R.9
Remennikov, G.10
Schimmel, H.11
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14
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0037241494
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H. Mayr, B. Kempf, A. R. Ofial, Acc. Chem. Res. 2003, 36, 66;
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Acc. Chem. Res.
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Mayr, H.1
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33745363641
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H. Mayr, A. R. Ofial, Angew. Chem. 2006, 118, 1876; Angew. Chem. Int. Ed. 2006, 45, 1844;
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Angew. Chem. 2006, 118, 1876; Angew. Chem. Int. Ed.
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Mayr, H.1
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78650476888
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N. Streidl, B. Denegri, O. Kronja, H. Mayr, Acc. Chem. Res. 2010, 43, 1537;
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Streidl, N.1
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79953729356
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H. Mayr, Angew. Chem. 2011, 123, 3692; Angew. Chem. Int. Ed. 2011, 50, 3612.
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Angew. Chem. 2011, 123, 3692; Angew. Chem. Int. Ed.
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Mayr, H.1
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19
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79953687397
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For different opinions toward the Mayr equation, see
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For different opinions toward the Mayr equation, see: T. W. Bentley, Angew. Chem. 2011, 123, 3688; Angew. Chem. Int. Ed. 2011, 50, 3608.
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Angew. Chem. 2011, 123, 3688; Angew. Chem. Int. Ed.
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Bentley, T.W.1
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20
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0037130639
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C. Schindele, K. N. Houk, H. Mayr, J. Am. Chem. Soc. 2002, 124, 11208;
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Schindele, C.1
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L. R. Domingo, P. Pérez, R. Contreras, Tetrahedron 2004, 60, 6585;
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Domingo, L.R.1
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9944225117
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R. Contreras, J. Andres, L. R. Domingo, R. Castillo, P. Pérez, Tetrahedron 2005, 61, 417;
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Contreras, R.1
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Fukui, K.1
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Sauer, J.1
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38
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84899851903
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For discussions of distortion energy in transition state within the context of FMO theory, see:
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For discussions of distortion energy in transition state within the context of FMO theory, see:
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-
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45
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77953109863
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For a recent discussion of diffusion controlled reactions using Mayr equation, see
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B. Braida, C. Walter, B. Engels, P. C. Hiberty, J. Am. Chem. Soc. 2010, 132, 7631. For a recent discussion of diffusion controlled reactions using Mayr equation, see
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Braida, B.1
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46
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84865431840
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J. Ammer, C. Nolte, H. Mayr, J. Am. Chem. Soc. 2012, 134, 13902.
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J. Am. Chem. Soc.
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Ammer, J.1
Nolte, C.2
Mayr, H.3
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47
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84899881826
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A, which could include many known and unknown factors affecting the activation energy, is a constant. So far, only the empirical valence band (EVB) method has been well developed to quantify LFER, see
-
A, which could include many known and unknown factors affecting the activation energy, is a constant. So far, only the empirical valence band (EVB) method has been well developed to quantify LFER, see
-
-
-
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50
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33845946492
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S. Braun-Sand, M. H. M. Olsson, A. Warshel, Adv. Phys. Org. Chem. 2005, 40, 201.
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Braun-Sand, S.1
Olsson, M.H.M.2
Warshel, A.3
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51
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84899818201
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A′ as a constant.
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A′ as a constant.
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-
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52
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84899871171
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A is also dependent on the set of electrophiles i. These electrophiles are similar but are differ mainly through electronic effects introduced by their different R substituents, which are far away from the reacting sites of the electrophiles (see also Scheme2).
-
A is also dependent on the set of electrophiles i. These electrophiles are similar but are differ mainly through electronic effects introduced by their different R substituents, which are far away from the reacting sites of the electrophiles (see also Scheme2).
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-
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53
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84899867974
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The LUMO orbitals here refer to the reacting orbitals responsible for the elecrophilicity. In calculations with different basis sets, these reaction orbitals could be changed to LUMO+1, LUMO+2 or others; in these cases, we have to use these corresponding reacting orbitals instead of the LUMO orbitals in Equation(6).
-
The LUMO orbitals here refer to the reacting orbitals responsible for the elecrophilicity. In calculations with different basis sets, these reaction orbitals could be changed to LUMO+1, LUMO+2 or others; in these cases, we have to use these corresponding reacting orbitals instead of the LUMO orbitals in Equation(6).
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54
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84899832226
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All of the geometry optimizations and frequency calculations were performed with the B3LYP functional and the 6-31G(d) basis set implemented in Gaussian03;
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All of the geometry optimizations and frequency calculations were performed with the B3LYP functional and the 6-31G(d) basis set implemented in Gaussian03;
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55
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84899794309
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Gaussian03 (RevisionC.02), M.J. Frisch, etal., Gaussian, Inc.: Pittsburgh, PA, 2004;
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Gaussian03 (RevisionC.02), M.J. Frisch, etal., Gaussian, Inc.: Pittsburgh, PA, 2004;
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0345491105
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C. Lee, W. Yang, R. G. Parr, Phys. Rev. B 1988, 37, 785;
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Lee, C.1
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61
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84899881092
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All discussed orbital energies are referred to the B3LYP/6-31G(d) values. We found that using orbital energies of HF/6-31G(d) and BP86/6-31G(g) gave the same conclusion (see the Supporting Information).
-
All discussed orbital energies are referred to the B3LYP/6-31G(d) values. We found that using orbital energies of HF/6-31G(d) and BP86/6-31G(g) gave the same conclusion (see the Supporting Information).
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63
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0000134807
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Y.-D. Wu, C.-L. Wong, K. W. K. Chan, G.-Z. Ji, X.-K. Jiang, J. Org. Chem. 1996, 61, 746.
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S. T. A. Berger, F. H. Seeliger, F. Hofbauer, H. Mayr, Org. Biomol. Chem. 2007, 5, 3020;
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36649019941
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F. Seeliger, S. T. A. Berger, G. Y. Remennikov, K. Polborn, H. Mayr, J. Org. Chem. 2007, 72, 9170;
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Seeliger, F.1
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0037016457
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R. Lucius, R. Loos, H. Mayr, Angew. Chem. 2002, 114, 97; Angew. Chem. Int. Ed. 2002, 41, 91;
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Angew. Chem. 2002, 114, 97; Angew. Chem. Int. Ed.
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Lucius, R.1
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55049121808
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33751555599
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S. Lakhdar, M. Westermaier, F. Terrier, R. Goumont, T. Boubaker, A. R. Ofial, H. Mayr, J. Org. Chem. 2006, 71, 9088.
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J. Org. Chem.
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Lakhdar, S.1
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33845943843
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F. Brotzel, B. Kempf, T. Singer, H. Zipse, H. Mayr, Chem. Eur. J. 2007, 13, 336.
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Chem. Eur. J.
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