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5Â¥2008-01-04 09:56:18
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PW91 Perdew-Wang generalized-gradient approximation Perdew and Wang (1992) BP Becke exchange plus Perdew correlation Becke (1988), Perdew and Wang (1992) PBE Perdew-Burke-Ernzerhof correlation Perdew et al. (1996) RPBE Revised PBE functional by Hammer et al. Hammer et al. (1999) HCTH Hamprecht, Cohen, Tozer and Handy functional Boese and Handy (2001) BLYP Becke exchange plus Lee-Yang-Parr correlation Becke (1988), Lee et al. (1988) BOP Becke One Parameter functional Tsuneda et al. (1999) VWN-BP BP functional with the local correlation replaced by the VWN functional. Vosko et al. (1980), Becke (1988), Perdew and Wang (1992) ÎÒÖ»¿´µ½Õâ¸ö¶«Î÷£¬»¹ÓÐÆäËûµÄ°ïÖúÂ𣿠|
6Â¥2008-01-04 12:06:43
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лл£¬Ó¦¸ÃÊÇÕâ¸ö°É VWN: The Vosko-Wilk-Nusair (VWN) functional is the most popular LSD correlation potential. It uses a fit to accurate numerical results (by Ceperly and Alder) of a uniform electron gas. Ceperley and Alder performed quantum Monte Carlo calculations on a uniform electron gas at low and high spin limits for several electron densities. VWN uses the Pade interpolation procedure to fit the CA results for both the para and ferro states and for low and high densities. DMol3 uses the best VWN (so called "Fit" parameters.PWC: The Perdew-Wang (PWC) functional is a recent parameterization of the Ceperley and Alder data, which corrects some VWN problems with fitting. PWC is the default functional for DMol3 calculations. The local spin-density (LSD) approximation accurately predicts structures, vibrations, and relative energies of covalent systems; however, bond energies are seriously overestimated. The local DFT should not be used for systems with weak bonds, such as hydrogen bonds. These problems with the LSD method can be corrected to a large extent by using the so-called gradient-corrected (or nonlocal) functionals. P91, BP, BLYP, BOP: DMol3 supports several nonlocal exchange and correlation functionals. The most popular, the Becke exchange functional (B88) is used in conjunction with the Perdew-Wang correlation functional (BP) or the Lee-Yang-Parr correlation functional (BLYP). The so-called generalized gradient corrected (GGA) functional, by Perdew and Wang (P91) was derived by considering low and high density regimes and by enforcing various summation rules. PBE: The PBE (Perdew, Burke and Enzerhof) functional (1996, 1997) is another GGA functional in which all the parameters (other then those in its LDA component) are fundamental constants. The exchange part of this functional is similar to the Becke formula (1986), and the correlation part is close to the Perdew-Wang functional (1986).This functional has a strong physical background, reliable numerical performance and it is frequently used in DFT calculations. RPBE: More recently, Hammer, Hansen and Norskov (1999) proposed a modified version of the PBE formula that improves considerably thermochemical results. So far this functional, called RPBE, has been mainly used for solids. HCTH: The HCTH functional, named for the authors' initials (Hamprecht et al., 1998), represents a "pragmatic" philosophy in designing a DFT functional. Assuming that the exact functional will never be found, they propose a flexible form of gradient corrected functional that is fitted to the training set of molecules. The default for the current implementation, the so called HCTH/407 functional, that was obtained by fitting to the set of the 407 atomic and molecular systems (Boese and Handy, 2001). This functional was found to predict a much improved thermochemistry for inorganic and hydrogen bonded systems. The standalone keyword for this functional is hcth407. The original HCTH-type functionals can be activated by keyword hcth93 (Hamprecht et al, 1998) and hcth147 (Boese et al. 2000). Although the NLSD methods are significantly better than the LSD method, particularly in studying chemical reactions, the NLSD methods may still lead to reaction barriers that are too low. VWN-BP: The VWN-BP functional is recommended for COSMO and COSMO-RS studies. |
7Â¥2008-01-04 12:18:32













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