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V - MSpace at the University of Manitoba

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Spin-orbit effects accounted for in <strong>the</strong> second term <strong>of</strong> equ<strong>at</strong>ion (2–14), where ��<br />

is <strong>the</strong> spin oper<strong>at</strong>or, can be ei<strong>the</strong>r included or neglected depending on <strong>the</strong> circumstances.<br />

A key benefit <strong>of</strong> this method is th<strong>at</strong> <strong>the</strong> mentioned singularities <strong>of</strong> <strong>the</strong> Breit-Pauli<br />

Hamiltonian, equ<strong>at</strong>ion (2–13), are avoided.<br />

2.2.3 Rel<strong>at</strong>ivistic Effective Core Potentials (RECPs)<br />

30<br />

��<br />

In <strong>the</strong> Schrödinger equ<strong>at</strong>ion for a valence orbital <strong>the</strong> one-electron Hamiltonian,<br />

equ<strong>at</strong>ion (2–15), includes <strong>the</strong> kinetic energy <strong>of</strong> <strong>the</strong> electron, <strong>the</strong> interactions <strong>of</strong> <strong>the</strong><br />

nucleus, and <strong>the</strong> core electrons, as well as <strong>the</strong> interactions with <strong>the</strong> o<strong>the</strong>r valence<br />

electrons and <strong>the</strong> rel<strong>at</strong>ivistic oper<strong>at</strong>or [27].<br />

H �<br />

� T �Vcore<br />

�Vnuc<br />

�Vrel<br />

Vval<br />

(2–15)<br />

With <strong>the</strong> RECP, <strong>the</strong> Schrödinger equ<strong>at</strong>ion (2–16) serves to replace <strong>the</strong> Coulomb<br />

effects <strong>of</strong> <strong>the</strong> inner core electrons, as well as <strong>the</strong> direct rel<strong>at</strong>ivistic effects on <strong>the</strong> valence<br />

electrons. In general, RECPs can be used with ei<strong>the</strong>r ab initio methods, including HF, or<br />

with DFT methods, to study molecules containing heavy elements. For <strong>the</strong> purposes <strong>of</strong><br />

this research RECPs were used only with <strong>the</strong> density functional method.<br />

��<br />

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