Hamiltonian Breit-Pauli spin-orbit

The Breit-Pauli spin-orbit Hamiltonian is found in many different forms in the literature. In expressions [101] and [102], we have chosen a form in which the connection to the Coulomb potential and the symmetry in the particle indices is apparent. Mostly s written in a short form where spin-same- and spin-other-orbit parts of the two-electron Hamiltonian have been contracted to a single term, either as... 

As may be seen by comparing Eqs. [103] and [105], the no-pair spin-orbit Hamiltonian has exactly the same structure as the Breit-Pauli spin-orbit Hamiltonian. It differs from the Breit-Pauli operator only by kinematical factors that damp the 1/rfj and l/r singularities. 

The electronic spin-orbit interaction operator, referred to as the Breit-Pauli spin-orbit Hamiltonian, is given by... 

In order to include the SOC effects, a suitable many-electron Hamiltonian should be introduced. We employed a widely used in calculations Breit-Pauli spin-orbit Hamiltonian ... 

The Breit—Pauli spin-orbit Hamiltonian is very useful for organic molecules when the matrix elements of are computed from the nonrelativistic wave functions using perturbation theory or response theory, but it often overestimates the magnitude of spin-orbit splitting. It also suffers from... 

Zimmerman and Kutateladze calculated spin-orbit coupling in linear l,n-diyl biradicals (n = 3 to 8) at the CASSCF(4,4)/3-21G level with the Breit-Pauli spin-orbit Hamiltonian and analyzed it using natural bond orbitals. For diyls with an even number of carbons, symmetry forces zero SOC, whereas for those with an odd number of carbons the main terms have like signs and add, providing a nonvanishing net SOC. The maximum SOC is found at 90° orientation... 

The first approximation method for the Breit-Pauli spin-orbit Hamiltonian is to neglect the contribution from the two-electron terms. Justification... 

Model core potential (MCP) methods replace core orbitals by a potential just as in ECP. On the other hand, MCP valence orbitals preserve the nodal structure of valence orbitals, unlike ECP valence orbitals. The expectation values of (r ) for the valence orbitals show that the results of MCP are closer to those calculated with all-electron orbitals when comparing MCP, ECP, and the all electron case. Comparisons between MCP and an all electron basis utilizing the full Breit-Pauli spin-orbit Hamiltonian based on multiconfigura-tional quasidegenerate perturbation theory (MCQDPT) calculations show good agreement between the two methods for hydrides of P, As, and Sb. The MCP based spin-orbit calculation appears to be a promising technique, but systematic studies of many different molecular systems are still needed to assess its characteristics and accuracy. 

First attempts to calculate molecular parity violating potentials within a two-component framework have been undertaken by Kikuchi and coworkers [168,169]. They have added the Breit-Pauli spin-orbit coupling operator Hso to the usual non-relativistic Hamiltonian Hq... 

In this section, the spin-orbit interaction is treated in the Breit-Pauli [13,24—26] approximation and incoi porated into the Hamiltonian using quasidegenerate perturbation theory [27]. This approach, which is described in [8], is commonly used in nuclear dynamics and is adequate for molecules containing only atoms with atomic numbers no larger than that of Kr. 

In Table I, 3D stands for three dimensional. The symbol symbol in connection with the bending potentials means that the bending potentials are considered in the lowest order approximation as already realized by Renner [7], the splitting of the adiabatic potentials has a p dependence at small distortions of linearity. With exact fomi of the spin-orbit part of the Hamiltonian we mean the microscopic (i.e., nonphenomenological) many-elecbon counterpart of, for example, The Breit-Pauli two-electron operator [22] (see also [23]). 

Neglecting spin-orbit contributions (smaller than other relativistic corrections for the ground state of atoms, and zero for closed-shell ones), the Breit hamiltonian in the Pauli approximation [25] (weak relativistic systems) can be written for a many electron system as ... 

The Breit-Pauli SOC Hamiltonian contains a one-electron and two-electron parts. The one-electron part describes an interaction of an electron spin with a potential produced by nuclei. The two-electron part has the SSO contribution and the SOO contribution. The SSO contribution describes an interaction of an electron spin with an orbital momentum of the same electron. The SOO contribution describes an interaction of an electron spin with the orbital momentum of other electrons. However, due to a complicated two-electron part, the evaluation of the Breit-Pauli SOC operator takes considerable time. A mean field approximation was suggested by Hess et al. [102] This approximation allows converting the complicated two-electron Breit-Pauli Hamiltonian to an effective one-electron spin-orbit mean-field form... 

The Breit-Pauli (BP) approximation [140] is obtained truncating the Taylor expansion of the Foldy-Wouthuysen (FW) transformed Dirac Hamiltonian [141] up to the (p/mc) term. The BP equation has the well-known mass-velocity, Darwin, and spin-orbit operators. Although the BP equation gives reasonable results in the first-order perturbation calculation, it cannot be used in the variational treatment. 

Table 3.1 Effective Nuclear Charge (Scaling Parameter) Z ff for Approximate Spin-Orbit Interaction Calculations Using the One-Electron Term in the Breit-Pauli Hamiltonian (Equation 3.8, developed by Koseki et...

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