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34250316110
-
-
We were unable to obtain 8 analytically pure and so did not obtain PES and IPES spectra.
-
We were unable to obtain 8 analytically pure and so did not obtain PES and IPES spectra.
-
-
-
-
19
-
-
34250307110
-
-
32.25MeCN (X.-H. Bu, K. Biradha, T. Yamaguchi, M. Nishimura, T. Ito, K. Tanaka, M. Shionoya, Chem. Commun. 2000, 1953) are not included, since these were rather imprecisely determined.
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32.25MeCN (X.-H. Bu, K. Biradha, T. Yamaguchi, M. Nishimura, T. Ito, K. Tanaka, M. Shionoya, Chem. Commun. 2000, 1953) are not included, since these were rather imprecisely determined.
-
-
-
-
20
-
-
34250361026
-
-
The structures of the radical ions of 6, in which there are a large number of degrees of freedom, could not be successfully minimised. Accordingly, we were also unable to calculate reorganisation energies and adiabatic values of IP and EA for this compound.
-
The structures of the radical ions of 6, in which there are a large number of degrees of freedom, could not be successfully minimised. Accordingly, we were also unable to calculate reorganisation energies and adiabatic values of IP and EA for this compound.
-
-
-
-
22
-
-
0346907277
-
-
For example, see: R. D. Hreha, C. P. George, A. Haldi, B. Domercq, M. Malagoli, S. Barlow, J.-L. Brédas, B. Kippelen, S. R. Marder, Adv. Funct. Mater. 2003, 13, 967. While the barrier is strictly ΔH†. ΔS† can be neglected due to similar vibrational degrees of freedom associated with the two adiabatic surfaces, meaning λ/4 is also a good estimate of the free-energy barrier, ΔG†.
-
For example, see: R. D. Hreha, C. P. George, A. Haldi, B. Domercq, M. Malagoli, S. Barlow, J.-L. Brédas, B. Kippelen, S. R. Marder, Adv. Funct. Mater. 2003, 13, 967. While the barrier is strictly ΔH†. ΔS† can be neglected due to similar vibrational degrees of freedom associated with the two adiabatic surfaces, meaning λ/4 is also a good estimate of the free-energy barrier, ΔG†.
-
-
-
-
23
-
-
0022004980
-
-
The reorganisation energy can also be obtained from a full vibrational analysis through summation of the contributions of the vibrational modes involved R. A. Marcus, N. Sutin, Biochim. Biophys. Acta 1985, 811, 265
-
The reorganisation energy can also be obtained from a full vibrational analysis through summation of the contributions of the vibrational modes involved (R. A. Marcus, N. Sutin, Biochim. Biophys. Acta 1985, 811, 265).
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34250320869
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This type of estimate assumes that the analyte and reference redox system show comparable solvation energies and comparable solid-state polarisation effects and ideally requires more or less reversible electrochemistry to ensure that the observed potential represents the thermodynamic potential. Moreover, differences in the magnitudes of solvation energies and solid-state polarisation effects mean that IPs arc best estimated from M+/M redox couples and a known IP, while EAs are best estimated from M/M- and a known EA. For example, we recently found that, in the case of 1,1-diaryl-2,3,4,5-tet- raphenylsiloles, use of [silole, silole, potentials, the TPD +/TPD potential and the IP of TPD gave EAs almost 1 eV more exothermic than the values obtained by direct measurement. See reference [26
-
+/TPD potential and the IP of TPD gave EAs almost 1 eV more exothermic than the values obtained by direct measurement. See reference [26].
-
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44
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34250352674
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These values are taken from J. E. Huheey, E. A. Keiter, R. L. Keiter, Inorganic Chemistry: Principles of Structure and Reactivity, 4th ed., Harper Collins, New York, 1993, p. 187. in which values according to a variety of other scales are also given.
-
These values are taken from J. E. Huheey, E. A. Keiter, R. L. Keiter, Inorganic Chemistry: Principles of Structure and Reactivity, 4th ed., Harper Collins, New York, 1993, p. 187. in which values according to a variety of other scales are also given.
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The compeling inductive and resonance effects of F and Cl can of course be gauged by Hammett coefficients. See for example J. March, Advanced Organic Chemistry, 3rd ed, Wiley, New York, 1985
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Gaussian 98 (Revision A.11), M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, V. G. Zakrzewski, J. A. Montgomery, R. E. Stratmann, J. C. Burant, S. Dapprich, J. M. Millam, A. D. Daniels, K. N. Kudin, M. C. Strain, O. Farkas, J. Tomasi, V. Barone, M. Cossi, R. Cammi, B. Mennucci, C. Pomelli, C. Adamo, S. Clifford, J. Ochterski, G. A. Petersson, P. Y. Ayala, Q. Cui, K. Morokuma, D. K. Malick, A. D. Rabuck, K. Raghavachari, J. B. Foresman, J. Cioslowski, J. V. Ortiz, B. B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I. Komaromi, R. Gomperts, R. L. Martin, D. J. Fox, T. Keith, M. A. Al-Laham, C. Y. Peng, A. Nanayakkara, C. Gonzalez, M. Challacombe, P. M. W. Gill, B. G. Johnson, W. Chen, M. W. Wong, J. L. Andres, M. Head-Gordon, E. S. Replogle, J. A. Pople, Gaussian, Inc., Pittsburgh, PA, 1998.
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Gaussian 03, Revision B.05, M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, J. A. Montgomery, Jr, T. Vreven, K. N. Kudin, J. C. Burant, J. M. Millam, S. S. Iyengar, J. Tomasi, V. Barone, B. Mennucci, M. Cossi, G. Scalmani, N. Rega, O.A. Petersson, H. Nakatsuji, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda, O. Kitao, H. Nakai, M. Klene, X. Li, J. E. Knox, H. P. Hratchian, J. B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R. E. Stratmann, O. Yazyev, A. J. Austin, R. Cammi, C. Pomelli, J. W. Ochterski, P. Y. Ayala, K. Morokuma, G. A. Voth, P. Salvador, J. J. Dannenberg, V. G. Zakrzewski, S. Dapprich, A. D. Daniels, M. C. Strain, O. Farkas, D. K. Malick, A. D. Rabuck, K. Raghavachari, J. B. Foresman, J. V. Ortiz, Q. Cui, A. G. Baboul, S. Clifford, J. Cioslowski, B. B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I. Komaromi, R. L. Martin, D. J. Fox, T. Keith, M. A. Al-Laham, C. Y. Peng, A. Nanayak
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Gaussian 03, Revision B.05, M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, J. A. Montgomery, Jr., T. Vreven, K. N. Kudin, J. C. Burant, J. M. Millam, S. S. Iyengar, J. Tomasi, V. Barone, B. Mennucci, M. Cossi, G. Scalmani, N. Rega, O.A. Petersson, H. Nakatsuji, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda, O. Kitao, H. Nakai, M. Klene, X. Li, J. E. Knox, H. P. Hratchian, J. B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R. E. Stratmann, O. Yazyev, A. J. Austin, R. Cammi, C. Pomelli, J. W. Ochterski, P. Y. Ayala, K. Morokuma, G. A. Voth, P. Salvador, J. J. Dannenberg, V. G. Zakrzewski, S. Dapprich, A. D. Daniels, M. C. Strain, O. Farkas, D. K. Malick, A. D. Rabuck, K. Raghavachari, J. B. Foresman, J. V. Ortiz, Q. Cui, A. G. Baboul, S. Clifford, J. Cioslowski, B. B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I. Komaromi, R. L. Martin, D. J. Fox, T. Keith, M. A. Al-Laham, C. Y. Peng, A. Nanayakkara, M. Challacombe, P. M. W. Gill, B. Johnson, W. Chen, M. W. Wong, C. Gonzalez, J. A. Pople, Gaussian, Inc., Wallingford CT, 2004.
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