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Quantum Chemistry / Quantum Mechanics Many-Particle Problems
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Angular Momentum p r
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Operator commutation properties:
z l lz do not commute y x knowing length and one projection is possible
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Spin of electron - relativistic property
in non-relativistic formalism: equivalent to a coordinate (x,y,z,sz) - also magnetic moment
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Fermions and bosons Enrico Fermi ( )
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Fermions and bosons Satyendra Nath Bose (1894-1974)
Enrico Fermi ( ) Satyendra Nath Bose ( )
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Many particle wavefunction for electrons:
Slater determinant: N = 2:
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The Born-Oppenheimer Approximation
.. nuclear SE .. electronic SE
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Atomic units me = 1 ħ = 1 1/(40) = 1 e = -1
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The Hartree-Fock approximation
orbitals HF equations: non-linear “one-particle”
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The Hartree-Fock approximation
nuclear attraction Exchange Coulomb (electron repulsion) kinetic
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Two-electron integrals
Coulomb Exchange - only for the same spins
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Linear combination of atomic orbitals, LCAO
spin part of the wavefunction spinorbital “molecular” orbital “atomic orbital”, AO MO expansion coefficient
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Roothan Equations HF equations in “AO” basis not linear - matrix form
solution: iteration electrons in “self-consistent field” (SCF) of the other Clemens C. J. Roothaan, * 1918
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Orbital terminology Molecular/atomic, MO, AO closed shell, open shell
lowest-unoccupied molecular orbital (LUMO) highest occupied molecular orbital (LUMO)
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“N4 catastrophe”
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AO basis sets Slater type orbitals, STO Gaussian type orbitals, GTO
“contraction” “primitive functions”
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Basis set ladder STO-3G, “minimal” 6-31G, “split valence”
6-31G*, 6-31G**, “polarization” G**, “diffuse” aug-cc-pVTZ aug-cc-pVQZ ....
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