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Computational Solid State Physics 計算物性学特論 第7回. 7. Many-body effect I Hartree approximation, H artree-Fock approximation and Density functional method. Hartree approximation. N-electron Hamiltonian . ・ N-electron wave function . i-th spin-orbit. ortho-normal set.
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Computational Solid State Physics 計算物性学特論 第7回 7.Many-body effect I Hartree approximation, Hartree-Fock approximation andDensity functional method
Hartree approximation N-electron Hamiltonian ・N-electron wave function i-th spin-orbit ortho-normal set
Expectation value of the energy single electron energy Hartreeinteraction
Charge density :charge density operator : charge density Hartree interaction
Hartree calculation for N>>1 Energy minimization with condition Self-consistent Schröedingerequation for the i-th state Electrostatic potential energy caused by electron-electron Coulomb interaction charge density
Hartree-Fock approximation • Pauli principle • Identical particles • Slater determinant • Exchange interaction • Hartree-Fock-Roothaan’s equation
Many electron Hamiltonian single electron Hamiltonian electron-electron Coulomb interaction
Slater determinant or N-electron wave function John Slater spin orbit Permutation of N numbers
Properties of Slater determinant or If Pauli principle Identical Fermi particles The Slater determinant satisfies both requirements of Pauli principle and identical Fermi particles on N-electron wave function.
Ground state energy Permutation of N numbers Orthonormal set
Expectation value of many-electron Hamiltonian Coulomb integral Exchange integral Hartree term: between like spin electrons and between unlike spin electrons Fock term: between like spin electrons
Exchange interaction Pauli principle X no transfer transfer No suppression of electron-electron Coulomb energy suppression of electron-electron Coulomb energy gain of exchange energy No exchange energy
Hartree-Fock calculation (1) Expansion by base functions
Hartree-Fock calculation (2) Calculation of the expectation value
Hartree-Fock calculation (3) Expectation value of N-electron Hamiltonian
Hartree-Fock calculation (4) Minimization of E with condition Hartree-Fock-Roothaan’s equation Exchange interaction is also considered in addition to electrostatic interaction.
Hartree-Fock calculation (5) Schröedinger equation for k-th state m: number of base functions N: number of electrons Self-consistent solution on C and P
Density functional theory • Density functional method to calculate the ground state of many electrons • Kohn-Sham equations to calculate the single particle state • Flow chart of solving Kohn-Sham equation
Many-electron Hamiltonian T: kinetic energy operator Vee: electron-electron Coulomb interaction vext: external potential
Variational principles • Variational principle on the ground state energy functional E[n]: The ground state energy EGSis the lowest limit of E[n]. • Representability of the ground state energy. :charge density
Hartree term Exchange correlation term Density-functional theory • Kohn-Sham total-energy functional for a set of doubly occupied electronic states
Kohn-Sham equations : Hartree potential of the electron charge density : exchange-correlation potential : excahnge-correlation functional
Kohn-Sham eigenvalues : Kinetic energy functional Janak’s theorem: If f dependence of εi is small, εimeans an ionization energy.
Local density approximation nX(r12) : Exchange-correlation energy per electron in homogeneous electron gas exchange hole distribution for like spin Local-density approximation satisfies the sum rule. Sum Rule: : exchange-correlation hole
Bloch’s theorem for periodic system G : Reciprocal lattice vectora :Lattice vector
Supercell geometry Point defect Surface Molecule
Flow chart describing the computational procedure for the total energy calculation Conjugate gradient method Molecular-dynamics method
Hellman-Feynman force on ions (1) : for eigenfunctions
Hellman-Feynman force on ions (2) Electrostatic force between ions Electrostatic force between an ion and electron charge density
Problems 7 • Derive the single-electron Schröedinger equations in Hartree approximation. • Derive the single-electron Schröedinger equations in Hartree-Fock approximation. • Derive the Kohn-Sham equation in density functional method. • Solve the sub-band structure at the interface of the GaAs active channel in a HEMT structure in Hartree approximation.