Approximation zeroth-order regular

Wolff, S. K., Ziegler, T., van Lenthe, E., Baerends, E. J., 1999, Density Functional Calculations of Nuclear Magnetic Shieldings Using the Zeroth-Order Regular Approximation (ZORA) for Relativistic Effects ZORA Nuclear Magnetic Resonance , J. Chem. Phys., 110, 7689. 

In this paper we present the first application of the ZORA (Zeroth Order Regular Approximation of the Dirac Fock equation) formalism in Ab Initio electronic structure calculations. The ZORA method, which has been tested previously in the context of Density Functional Theory, has been implemented in the GAMESS-UK package. As was shown earlier we can split off a scalar part from the two component ZORA Hamiltonian. In the present work only the one component part is considered. We introduce a separate internal basis to represent the extra matrix elements, needed for the ZORA corrections. This leads to different options for the computation of the Coulomb matrix in this internal basis. The performance of this Hamiltonian and the effect of the different Coulomb matrix alternatives is tested in calculations on the radon en xenon atoms and the AuH molecule. In the atomic cases we compare with numerical Dirac Fock and numerical ZORA methods and with non relativistic and full Dirac basis set calculations. It is shown that ZORA recovers the bulk of the relativistic effect and that ZORA and Dirac Fock perform equally well in medium size basis set calculations. For AuH we have calculated the equilibrium bond length with the non relativistic Hartree Fock and ZORA methods and compare with the Dirac Fock result and the experimental value. Again the ZORA and Dirac Fock errors are of the same order of magnitude. 

Within the DFT framework, we apply two different approaches to deal with relativistic effects, the so-called quasi-relativistic (QR) method (73) and the more modem "Zeroth Order Regular Approximation for Relativistic Effects" (ZORA) (14-16). The QR method is also known as the Pauli approach. 

Autschbach and Ziegler performed the relativistic calculations of spin-spin coupling constants (isotropic part) and anisotropies in heavy atom compounds with the two-component zeroth-order regular approximation (ZORA) method. The experimentally determined reduced spin-spin coupling tensor elements Kjk A,B) between two magnetically active nuclei, A and... 

Table 4.13 Distance of C atom to closest Pt atom in the surface (Rpt-c) and binding energy ( b) for CO adsorbed on Pt(l 11) in the on-top position RDVM results versus complete active space self-consistent-field data (CASSCF) (Roszak and Balasubramanian 1995) and GGA results within the zeroth-order regular approximation (ZDRA) (Philipsen et al. 1997). Exp. Ogletree et al. (1986).

ZORA zeroth-order regular approximation, also known as CPD (for Chang-Pelissier-Durand)... 

One-component calculations or two-component calculations including also spin-orbit coupling effects provide a firm basis for the calculations of higher-order relativistic corrections by means of perturbation theory. Several quasi-relativistic approximations have been proposed. The most successful approaches are the Douglas-Kroll-Hess method (DKH) [1-7], the relativistic direct perturbation theory (DPT) [8-24], the zeroth-order regular approximation (ZORA) [25-48], and the normalized elimination of small components methods (NESC) [49-53]. Related quasi-relativistic schemes based on the elimination of the small components (RESC) and other similar nonsingular quasi-relativistic Hamiltonians have also been proposed [54-61]. 

Another method to avoid the singularities in the vicinity of the nuclei was proposed by van Lenthe et al. [26,27,35]. They suggested an method that also includes the interaction potential, V (r), in the denominator of the ansatz for the small component. This ansatz was used in the derivation of the so called zeroth-order regular approximation (ZORA) Hamiltonian. The ZORA ansatz can thus be the written as... 

Figure 1. The Exponential Regular Approximation (ERA with y= 1), the Zeroth-Order-Regular Approximation (ZORA), and the Kinetic-Energy Balance Condition (KEBC) ansatz functions for uranium (Z = 92). The distance R is given in bohrs.

The zeroth-order regular approximation (ZORA) Hamiltonian can be derived from the upper part of the transformed Dirac equation (20). By using the ZORA ansatz for the small component (5) and assuming that the upper and the lower components are equal, the final ZORA equation for the upper component becomes... 

One of the shortcomings of the BP approach is that the expansion in (p/mc) is not justified in the case where the electronic momentum is too large, e.g. for a Coulomb-like potential. The zeroth-order regular approximation (ZORA) [142,143] can avoid this disadvantage by expanding in E/ 2mc — P) up to the first order. The ZORA Hamiltonian is variationally stable. However, the Hamiltonian obtained by a higher order expansion has to be treated perturbatively, similarly to the BP Hamiltonian. Other quasi-relativistic methods have been proposed by Kutzelnigg [144,145] and DyaU [146]. 

Three quasi-relativistic approaches that are variationally stable are the Doug-lass-Kroll-Hess transformation of the no-pair Hamiltonian (for example, see Ref. 11, 20, 23-29), the zeroth order regular approximation, ZORA, (for example, see Ref. 30-34), and the approach of Barysz and Sadlej (for example, see Ref. 36). The results of the first two approaches differ considerably even when used by the same authors,which led them to try the third approach. A calibration study suggests that relativistic effects on heavy atom shieldings are significantly underestimated by ZORA in comparison to the four-component relativistic treatment, but that the neighboring proton chemical shifts are closer to experi-... 

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