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The Becke3LYP functional combines Becke's hybrid exchange functional [A. D. Becke, J. Chem. Phys. 98, 5648 (1993)] and the LYP correlation functional [C. Lee, W. Yang, R. G. Parr, Phys. Rev. B 37, 785 (1988)], with the weights of the various terms in the functional being the default values in Gaussian 94. The 6-31 +G[d,p] basis set combines the 6-31 +G basis set with the diffuse polarization functions from the aug-cc-pVDZ set [R. A. Kendall, T. H. Dunning Jr., R. J. Harrison, J. Chem. Phys. 96, 6796 (1992)].
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Becke, A.D.1
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23
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0345491105
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The Becke3LYP functional combines Becke's hybrid exchange functional [A. D. Becke, J. Chem. Phys. 98, 5648 (1993)] and the LYP correlation functional [C. Lee, W. Yang, R. G. Parr, Phys. Rev. B 37, 785 (1988)], with the weights of the various terms in the functional being the default values in Gaussian 94. The 6-31 +G[d,p] basis set combines the 6-31 +G basis set with the diffuse polarization functions from the aug-cc-pVDZ set [R. A. Kendall, T. H. Dunning Jr., R. J. Harrison, J. Chem. Phys. 96, 6796 (1992)].
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Lee, C.1
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24
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4143095330
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-
The Becke3LYP functional combines Becke's hybrid exchange functional [A. D. Becke, J. Chem. Phys. 98, 5648 (1993)] and the LYP correlation functional [C. Lee, W. Yang, R. G. Parr, Phys. Rev. B 37, 785 (1988)], with the weights of the various terms in the functional being the default values in Gaussian 94. The 6-31 +G[d,p] basis set combines the 6-31 +G basis set with the diffuse polarization functions from the aug-cc-pVDZ set [R. A. Kendall, T. H. Dunning Jr., R. J. Harrison, J. Chem. Phys. 96, 6796 (1992)].
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Kendall, R.A.1
Dunning Jr., T.H.2
Harrison, R.J.3
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25
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84986468715
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T. Clark, J. Chandrasekhar, G. W. Spitznagel, P. v. R Schleyer, J. Comp. Chem. 4, 294 (1983); W. J. Hehre, R. Ditchfield, J. A. Pople, J. Chem. Phys. 56, 2257 (1972); M. J. Frisch, J. A. Pople, J. S. Binkley, ibid. 80, 3265 (1984).
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26
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0347170005
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Hehre, W.J.1
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36549091139
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29
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1842305840
-
-
note
-
Previous work (12, 20, 22) has demonstrated that DFT calculations using the Becke3LYP functional faithfully reproduce the trends in the OH stretch spectra of water and benzene-water clusters. The major deficiency of such calculations is an exaggeration of the magnitude of the shifts of the single-donor OH stretch frequencies.
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-
30
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0001188328
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J. E. Del Bene, W. B. Person, K. Szczepaniak, J. Phys. Chem. 99, 10705 (1995); S. S. Xantheas, J. Chem. Phys. 102, 4595 (1995).
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Del Bene, J.E.1
Person, W.B.2
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31
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0001188328
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J. E. Del Bene, W. B. Person, K. Szczepaniak, J. Phys. Chem. 99, 10705 (1995); S. S. Xantheas, J. Chem. Phys. 102, 4595 (1995).
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Xantheas, S.S.1
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33
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1842380923
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4) is available on the World Wide Web at http://www.pitt.edu/∼jordan/science_article/ BW8/table
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34
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1842346050
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note
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We gratefully acknowledge NSF for support of this research from grants CHE-9404716 and CHE-9422210. We thank C. Sosa of Silicon Graphics and Cray Research for assistance with some of the calculations.
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