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Scalmani, G.2
Rega, N.3
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90
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34547805718
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Zalatan, J. G.; Catrina, I.; Mitchell, R.; Grzyska, P. K.; O'Brien, P. J.; Herschlag, D.; Hengge, A. C. J. Am. Chem. Soc. 2007, 129, 9789-9798
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Herschlag, D.6
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0242593713
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Tao, J.; Perdew, J. P.; Staroverov, V. N.; Scuseria, G. E. Phys. Rev. Lett. 2003, 91, 146401
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99
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79952274311
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note
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m are the rate constant, Boltzmann constant, Planck constant, universal gas constant, absolute temperature and active free energy in the standard state of a mole particles, respectively.
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100
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0007671378
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Bach, R. D.; Gonzales, C.; Andres, J. L.; Schlegel, H. B. J. Org. Chem. 1995, 60, 4653-4656
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Bach, R.D.1
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Andres, J.L.3
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101
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13044253676
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Lewis, D. E.; Sims, L. B.; Yamataka, H.; McKenna, J. J. Am. Chem. Soc. 1980, 102, 7411-7419
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Lewis, D.E.1
Sims, L.B.2
Yamataka, H.3
McKenna, J.4
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107
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79952269820
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In the absence of catalyst, the EIEs (1.0245 and 1.0002) for deprotonation of HpPNP were calculated using the program ISOEFF98 with PCM/B3LYP/6-31+G(d,p) by Hengge and co-workers (ref 28). We also recalculated the EIEs at the level of PCM/B3LYP/6-31G(d,p) within the harmonic oscillator/rigid rotor approximations, as implemented in the Gaussian 03 program. Our results are similar to the values of ref 28.
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In the absence of catalyst, the EIEs (1.0245 and 1.0002) for deprotonation of HpPNP were calculated using the program ISOEFF98 with PCM/B3LYP/6-31+G(d,p) by Hengge and co-workers (ref 28). We also recalculated the EIEs at the level of PCM/B3LYP/6-31G(d,p) within the harmonic oscillator/rigid rotor approximations, as implemented in the Gaussian 03 program. Our results are similar to the values of ref 28.
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110
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79952262199
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+
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+.
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111
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0034812442
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Velikyan, I.; Acharya, S.; Trifonova, A.; Földesi, A.; Chattopadhyaya, J. J. Am. Chem. Soc. 2001, 123, 2893-2894
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(2001)
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Velikyan, I.1
Acharya, S.2
Trifonova, A.3
Földesi, A.4
Chattopadhyaya, J.5
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112
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4344672759
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Lönnberg, H.; Strömberg, R.; Williams, A. Org. Bimmol. Chem. 2004, 2, 2165-2167
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(2004)
Org. Bimmol. Chem.
, vol.2
, pp. 2165-2167
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Lönnberg, H.1
Strömberg, R.2
Williams, A.3
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113
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79952255711
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a values (ref 67) are about 13, and in 298.15K, the rough free energy change values are approximately estimated to be about 17.7 kcal/mol.
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a values (ref 67) are about 13, and in 298.15K, the rough free energy change values are approximately estimated to be about 17.7 kcal/mol.
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114
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79952267026
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The sum of the bond orders to the nucleophile and leaving group is less than 1 in a loose transition state, while this sum is greater than 1 in a tight (or associative) transition state (see refs 54a and 54c for details).
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The sum of the bond orders to the nucleophile and leaving group is less than 1 in a loose transition state, while this sum is greater than 1 in a tight (or associative) transition state (see refs 54a and 54c for details).
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115
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79952256191
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The orbital interaction energies are roughly estimated by the second order perturbation theory analysis of the Fock Matrix in a NBO basis.
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The orbital interaction energies are roughly estimated by the second order perturbation theory analysis of the Fock Matrix in a NBO basis.
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116
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79952255837
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In Fan and Gao's work (ref 45), the TPSS density functional theory (with density fitting functions included) was employed. The basis set 6-31++G(d′,p′) was used for N, O, aromatic C, and all H atoms bound to N and O, while 6-31G was used for alkyl C and the rest of all H atoms, SDD was used for Zn atoms, and LANL2DZ plus a d-polarization, and a p-diffuse function was used for P atom.
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In Fan and Gao's work (ref 45), the TPSS density functional theory (with density fitting functions included) was employed. The basis set 6-31++G(d′,p′) was used for N, O, aromatic C, and all H atoms bound to N and O, while 6-31G was used for alkyl C and the rest of all H atoms, SDD was used for Zn atoms, and LANL2DZ plus a d-polarization, and a p-diffuse function was used for P atom.
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