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LDA Limitations

Measuring denser dispersed flows, the solid- and fluid particles may block the required transparent light paths and the light may also be reflected on fluid particle surfaces which prevent valid signals. The application of the LDA technique is thus limited to dilute dispersions. [Pg.1290]


It is important to note that the only physical approximation here is the LDA. All other approximations are of a numerical nature and their convergence can be monitored and improved in a systematic way. Thus, this method allows a probe of the LDA limit for molecules and clusters without any further approximations such... [Pg.53]

Any function of two electron densities pa and ps), their gradients VPa and Vpe), and higher derivatives V2Pa and V2ps, etc.), can be used to approximate Tfad[pA- Pb - Obeying the LDA limit restricts the form the approximate functional to ... [Pg.23]

These equations are called the generalized-gradient-approximation (GGA) limit conditions, and, in particular, the x = 0 values of these energies are called the local density approximation (LDA) limit conditions. Here, it should be noted that the coefficient of the x term in the exchange energy expansion in Eq. (8.5) is twice the conventional value (Kleinman and Lee 1988). The reason for this difference is mentioned later. [Pg.190]

The most common conditions employed in the Madelung process are sodium/potassium alkoxide or sodium amide at elevated temperature (200-400 C). The Madelung reaction could be effected at lower temperature when -BuLi or LDA are employed as bases/ The useful scope of the synthesis is, therefore, limited to molecules which can survive strongly basic conditions. The process has been successfully applied to indoles bearing alkyl substituents. ... [Pg.141]

Dickson and Becke, 1996, use a basis set free numerical approach for obtaining their LDA dipole moments, which defines the complete basis set limit. In all other investigations basis sets of at least polarized triple-zeta quality were employed. Some of these basis sets have been designed explicitly for electric field response properties, albeit in the wave function domain. In this category belong the POL basis sets designed by Sadlej and used by many authors as well as basis sets augmented by field-induced polarization (FTP) func-... [Pg.196]

If the main limitations of HF theory are overcome by the introduction of electron correlation, those of density functional theory are expanded by the use of more accurate functionals. These functionals, that improve the uniform gas description of the LDA approach, are labeled as non-local or Generalize Gradient Approximation (GGA). [Pg.10]

Successful lithiation of aryl halides—carbocyclic or heterocyclic—with alkyUithiums is, however, the exception rather than the rule. The instability of ortholithiated carbocyclic aryl halides towards benzyne formation is always a limiting feature of their use, and aryl bromides and iodides undergo halogen-metal exchange in preference to deprotonation. Lithium amide bases avoid the second of these problems, but work well only with aryl halides benefitting from some additional acidifying feature. Chlorobenzene and bromobenzene can be lithiated with moderate yield and selectivity by LDA or LiTMP at -75 or -100 °C . [Pg.540]

Nonempirical GGA functionals satisfy the uniform density limit. In addition, they satisfy several known, exact properties of the exchange-correlation hole. Two widely used nonempirical functionals that satisfy these properties are the Perdew-Wang 91 (PW91) functional and the Perdew-Burke-Ernzerhof (PBE) functional. Because GGA functionals include more physical ingredients than the LDA functional, it is often assumed that nonempirical GGA functionals should be more accurate than the LDA. This is quite often true, but there are exceptions. One example is in the calculation of the surface energy of transition metals and oxides. [Pg.217]

In this paper we present preliminary results of an ab-initio study of quantum diffusion in the crystalline a-AlMnSi phase. The number of atoms in the unit cell (138) is sufficiently small to permit computation with the ab-initio Linearized Muffin Tin Orbitals (LMTO) method and provides us a good starting model. Within the Density Functional Theory (DFT) [15,16], this approach has still limitations due to the Local Density Approximation (LDA) for the exchange-correlation potential treatment of electron correlations and due to the approximation in the solution of the Schrodinger equation as explained in next section. However, we believe that this starting point is much better than simplified parametrized tight-binding like s-band models. [Pg.536]


See other pages where LDA Limitations is mentioned: [Pg.136]    [Pg.120]    [Pg.108]    [Pg.108]    [Pg.21]    [Pg.194]    [Pg.194]    [Pg.194]    [Pg.195]    [Pg.1290]    [Pg.136]    [Pg.120]    [Pg.108]    [Pg.108]    [Pg.21]    [Pg.194]    [Pg.194]    [Pg.194]    [Pg.195]    [Pg.1290]    [Pg.2226]    [Pg.331]    [Pg.151]    [Pg.140]    [Pg.143]    [Pg.148]    [Pg.171]    [Pg.221]    [Pg.88]    [Pg.15]    [Pg.101]    [Pg.194]    [Pg.274]    [Pg.208]    [Pg.228]    [Pg.228]    [Pg.1185]    [Pg.1231]    [Pg.217]    [Pg.142]    [Pg.32]    [Pg.93]    [Pg.144]    [Pg.148]    [Pg.168]    [Pg.411]    [Pg.532]   


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