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Coulomb repulsion and Slater Integrals
Maurits W. Haverkort Institute for theoretical physics – Heidelberg University
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The Coulomb Integral is nasty: The integrant diverges at r1=r2
Coulomb Hamiltonian: In order to create the Hamiltonian as a matrix we need to evaluate the following integral Solution by Slater: Expand the operator on Spherical Harmonics. Solve the angular part analytical and the Radial integral numerical (Slater Integrals.) Also works in solids. (Spherical Harmonics are not eigen-states, but still a valid basis set.
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Coulomb interaction – Slater Integrals
Expansion on renormalized Spherical Harmonics with Useful expansion because our basis functions are (close to) spherical
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Coulomb interaction – Slater Integrals
Integral to calculate Expansion on renormalized Spherical Harmonics
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Coulomb interaction – Slater Integrals
Radial part: Slater integrals Angular part: Analytical solution
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Coulomb interaction – Slater Integrals
Graphical representation
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Coulomb interaction – Slater Integrals
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Coulomb interaction – Slater Integrals
Triangular equations
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Coulomb interaction – Slater Integrals
Parity
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Coulomb interaction – Slater Integrals
d - electrons
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Coulomb interaction – Slater Integrals
f - electrons
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Coulomb interaction – Slater Integrals
Core (p) valence (d) interaction – direct term
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Coulomb interaction – Slater Integrals
Core (p) valence (d) interaction – exchange term
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