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Volumn 112, Issue 2, 2008, Pages 467-482

An improved multistate empirical valence bond model for aqueous proton solvation and transport

Author keywords

[No Author keywords available]

Indexed keywords

BINDING ENERGY; COMPUTER SIMULATION; MOLECULAR DYNAMICS; QUANTUM THEORY; SOLVATION;

EID: 38749111812     PISSN: 15206106     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp076658h     Document Type: Article
Times cited : (226)

References (90)
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    • (1986) The Chemical Physics of Solvation
    • Zundel, G.1    Fritsch, J.2
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    • Frisch, M. J, Trucks, G. W, Schlegel, H. B, Scuseria, G. E, Robb, M. A, Cheeseman, J. R, Montgomery, J. A, Vreven, J, Kudin, T, Burant, K. N, Millam, J. C, Iyengar, J. M, Tomasi, S. S, Barone, J, Mennucci, V, Cossi, B, Scalmani, M, Rega, G, Petersson, N, Nakatsuji, G. A, Hada, H, Ehara, M, Toyota, M, Fukuda, K, Hasegawa, R, Ishida, J, Nakajima, M, Honda, T, Kitao, Y, Nakai, O, Klene, H, Li, M, Knox, X, Hratchian, J. E, Cross, H. P, Bakken, J. B, Adamo, V, Jaramillo, C, Gomperts, J, Stratmann, R, Yazyev, R. E, Austin, O, Cammi, A. J, Pomelli, R, Ochterski. C, Ayala, J. W, Morokuma, P. Y, Voth, K, Salvador, G. A, Dannenberg, P, Zakrzewski, J. J, Dapprich, V. G, Daniels, S, Strain, A. D, Farkas, M. C, Malick, O, Rabuck, D. K, Raghavachari, A. D, Foresman, K, Ortiz, J. B, Cui, J. V, Baboul, Q, Clifford, A. G, Cioslowski, S, Stefanov, J, Liu, B. B, Liashenko, G, Piskorz, A, Komaromi, P, Martin, I, Fox, R. L, Keith, D. J
    • Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.; Cheeseman, J. R.; Montgomery, J. A.; Vreven, J.; Kudin, T.; Burant, K. N.; Millam, J. C.; Iyengar, J. M.; Tomasi, S. S.; Barone, J.; Mennucci, V.; Cossi, B.; Scalmani, M.; Rega, G.; Petersson, N.; Nakatsuji, G. A.; Hada, H.; Ehara, M.; Toyota, M.; Fukuda, K.; Hasegawa, R.; Ishida, J.; Nakajima, M.; Honda, T.; Kitao, Y.; Nakai, O.; Klene, H.; Li, M.; Knox, X.; Hratchian, J. E.; Cross, H. P.; Bakken, J. B.; Adamo, V.; Jaramillo, C.; Gomperts, J.; Stratmann, R.; Yazyev, R. E.; Austin, O.; Cammi, A. J.; Pomelli, R.; Ochterski. C.; Ayala, J. W.; Morokuma, P. Y.; Voth, K.; Salvador, G. A.; Dannenberg, P.; Zakrzewski, J. J.; Dapprich, V. G.; Daniels, S.; Strain, A. D.; Farkas, M. C.; Malick, O.; Rabuck, D. K.; Raghavachari, A. D.; Foresman, K.; Ortiz, J. B.; Cui, J. V.; Baboul, Q.; Clifford, A. G.; Cioslowski, S.; Stefanov, J.; Liu, B. B.; Liashenko, G.; Piskorz, A.; Komaromi, P.; Martin, I.; Fox, R. L.; Keith, D. J.; Al-Laham, T.; Peng, M. A.; Nanayakkara, C. Y.; Challacombe, A.; Gill, M.; Johnson, P. M. W.; Chen, B.; Wong, W.; Gonzalez, M. W.; Pople, J. A. Gaussian 03, revision, C.02; Gaussian, Inc.: Wallingford, CT, 2004.
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    • It may be helpful to clarify the meaning of the last donor through an example. For instance, consider a pivot hydronium-identity sequence: 1-2-3-2-3. The last donor for each step in this sequence is null, 1, 2, 1, 2, in the same order. Note that, when the proton hops back to 2 from 3, the last donor is 1 instead of 3, because 1 was the molecule from which the proton originally hopped to 2. Therefore, h(δt) for each step is 0, 1, 2, 1, 2, in that order.
    • It may be helpful to clarify the meaning of the "last donor" through an example. For instance, consider a pivot hydronium-identity sequence: 1-2-3-2-3. The "last donor" for each step in this sequence is null, 1, 2, 1, 2, in the same order. Note that, when the proton hops back to 2 from 3, the last donor is 1 instead of 3, because 1 was the molecule from which the proton originally hopped to 2. Therefore, h(δt) for each step is 0, 1, 2, 1, 2, in that order.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.