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Molecular results

Atomization energies (in a.u.), bond lengths (in A), and force constants k of the breathing mode (in a.u.), from one-component SCF calculations using energy-consistent scalar-relativistic pseudopotentials (EC-PP), ab initio model potentials (AIMP) and valence basis sets of double zeta (DZ) and polarized double-zeta (DZP) quality, in comparison to all-electron (AE) relativistic SCF calculations. Numbers in parentheses are differences to corresponding non-relativistic results. [Pg.848]

The performance of energy-consistent quasirelativistic 7-valence electron PPs for all halogen elements has been investigated in a study of the monohydrides and homonuclear dimers [242]. Special attention was also paid to the accuracy of valence correlation energies obtained with pseudo valence orbitals [97,98]. Some of the results for the halogen dimers is presented in Tables 13 [Pg.849]

Bond lengths R (A), binding energies D. (eV) and vibrational constants a e (cm ) of the homonuclear halogen dimers from dl-electron (AE) Douglas-Kroll-HeB (DKH) and valence-only energy-consistent pseudopotential (EC-PP) Hartree-Fock self-consistent field (SCF) calculations. The effects of static and dynamic core-polarization at the valence-only level are modelled by a core-polarization potential (CPP). [Pg.850]

In contrast to main group elements and d-transition metals accurate exper- [Pg.851]


DMI resistance may be governed by different resistance mechanisms co-existing in the same isolate. Molecular detection tools can help to find low frequencies of mutated individuals in populations. However, since resistance to DMIs may be a combined effect of several mechanisms, the molecular results have to be treated with care and bioassays may be always needed for verification. [Pg.80]

Radhakrishnan and co-workers [6] also studied the freezing of CCI4 in activated carbon fibers (ACF) of uniform nano-scale structures, using Monte Carlo simulation and differential scanning calorimetry (DSC), klicro-porous activated carbon fibers serve as highly attractive adsorbents for simple non-polar molecules. The DSC experiments verified the predictions about the increase in T/. and the molecular results were consistent with equation (1) for pore widths in the mesoporous range they also explained the deviation from the linear behavior in the case of micropores. [Pg.142]

The origin of shape-consistent pseudopotentials [131,160] lies in the insight that the admixture of only core orbitals to valence orbitals in order to remove the radial nodes leads to too contracted pseudo valence orbitals and finally as a consequence to poor molecular results, e.g., to too short bond distances. It has been recognized about 20 years ago that it is indispensable to have the same shape of the pseudo valence orbital and the original valence orbital in the spatial valence region, where chemical bonding occurs. Formally this requires also an admixture of virtual orbitals in Eq. 37. Since these are usually not obtained in finite difference atomic calculations, another approach was developed. Starting point... [Pg.821]

Eukarya is a group of organisms with a membrane-bound nucleus. They are multicellular and diverse in species machinery. Some eukaryotes have sexual reproduction, and gene exchange can occur also by transduction and transformation. Genetic information is based on several complex RNA polymerases, and translation starts with methionine. Eukarya was long considered as the third major domain of the life tree. Current molecular results... [Pg.300]

Colton has described FAB as a method that provides the molecular results of static SIMS under the high-flux conditions of dynamic SIMS. It is now understood that the important feature of this technique is the liquid matrix, and not the neutral beam. Thus, the technique is more appropriately described as liquid SIMS. The liquid... [Pg.102]

Different models were assessed for the electronegativity and chemical hardness as well, namely the experimental based finite-difference (FZ)) (Mulliken, 1934 Lackner Zweig, 1983), Putz-DFT (Putz, 2006), and Putz-SC (semiclassical) (Putz, 2007b) ones. The atomic values for atoms involved are displayed in Table 3.29, while the molecular results, based... [Pg.378]

As mentioned above, the PCI-X method was originally designed for the treatment of transition metal system. Therefore this procedure has to be tested for this kind of system too. The first test of the PQ-80 scheme on transition metal systems is performed on the atomic spectra, which is the only set of very accurate experimental data available. The s s° excitation was calculated for the neutral second row transition metal atoms and the first row transition metal cations, The s -> s excitation was calculated for both the first and the second row neutral transition metal atoms. In Table 3 we summarize the mean absolute deviation from experimental data on these excitations at the MCPF and the PCI-80 levels. A few technical comments on the results in Table 3 should be made. The first comment concerns the s states. As already noted above for first row atoms, valence excitations from s to p introduce additional problems. To avoid this problem for the s states of the transition metal atoms, the correlation energy associated with these two electrons is excluded from the extrapolation procedure. This somewhat awkward procedure was used to obtain the results in Table 3. but is entirely restricted to these atomic calculations. To avoid this problem for the molecular bond strengths, the calculated s asymptote should be used and experimental excitation energies should be used to obtain the final bond strengths. This has been done for most of the molecular results given below. Second, in... [Pg.500]

This section summarizes the earlier molecular results [18]. FFs/+ and f were computed for 23 molecules at geometries optimized with the DND basis and VWN potential. Table 7.1 lists the RMS differences relative to the VWN/DND/AAf = 0.1 results for AAf = 0.01 and AA = 1.0. Many of the atomic FFs are quite small, on the order of 0.01-0.05. Consequently, very small differences in the results can inflate the RMS values. For this reason, the results in Table 7.1 comprise only the chemically significant FFs, which are arbitrarily taken as/+ > 0.10. [Pg.104]

Molecular Results Average RMS Difference (%) for Atomic FFs Compared to A/V = 0.1... [Pg.105]


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