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4.2 Hartree-Fock Method and Self-Consistent Field

4 min readaugust 14, 2024

The tackles many-electron systems by approximating each electron's motion in an average field of others. It uses a variational approach to find the best single-determinant wave function, balancing accuracy with computational efficiency.

The self-consistent field process iteratively refines the electron until convergence. While it neglects instantaneous electron correlation, this method provides valuable insights into atomic structure and properties, forming a foundation for more advanced quantum chemistry techniques.

Hartree-Fock Method

Variational Approach and Effective Potential

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  • The Hartree-Fock method is a variational approach to approximating the ground state wave function and energy of a multi-electron system
  • It assumes that each electron moves independently in an effective potential created by the nuclei and the average field of all other electrons ()
  • The Hartree-Fock method employs the Born-Oppenheimer approximation, which separates the motion of electrons from that of the nuclei, allowing for the treatment of electronic motion independently

Wave Function Approximation and Minimization

  • The wave function is approximated as a product of single-electron wave functions (orbitals), known as a , to ensure the antisymmetry of the total wave function
    • Antisymmetry is required to satisfy the , which states that no two electrons can occupy the same quantum state simultaneously
  • The method involves minimizing the energy of the system with respect to the single-electron wave functions, subject to the constraint that they remain orthonormal
  • The Hartree-Fock equations are derived by applying the to the energy expectation value, leading to a set of coupled integro-differential equations

Self-Consistent Field

Iterative Process

  • The is the effective potential experienced by each electron due to the nuclei and the average field of all other electrons
  • In the Hartree-Fock method, the SCF is determined iteratively until is achieved
  • The iterative process begins with an initial guess for the single-electron wave functions (orbitals)
  • Using these initial orbitals, the Coulomb and exchange potentials are calculated, which together form the SCF
    • The represents the classical electrostatic repulsion between electrons
    • The arises from the quantum-mechanical requirement of antisymmetry and has no classical analog

Convergence and Best Approximation

  • The Hartree-Fock equations are then solved using the SCF to obtain a new set of orbitals
  • The process is repeated, using the new orbitals to update the SCF, until the change in the orbitals and the total energy between iterations falls below a predefined threshold (convergence)
    • are typically based on the change in the total energy and the maximum change in the orbital coefficients
  • Upon convergence, the resulting orbitals and their corresponding energies represent the best single-determinant approximation to the true wave function and energy within the Hartree-Fock framework

Hartree-Fock Approximations

Electron Correlation and Accuracy

  • The Hartree-Fock method neglects the instantaneous correlation between electrons, as it considers each electron to move in an average field of all other electrons
    • Instantaneous correlation refers to the fact that electrons avoid each other due to their mutual Coulomb repulsion
  • The method overestimates the electron-electron repulsion energy and underestimates the total energy compared to the exact solution
  • The accuracy of the Hartree-Fock method decreases for systems with significant electron correlation, such as molecules with partially filled degenerate orbitals (transition metal complexes) or those undergoing bond dissociation

Relativistic Effects and Basis Sets

  • The Hartree-Fock method does not account for relativistic effects, which can be important for heavy atoms (gold, mercury) or high-precision calculations
  • The choice of the (the mathematical functions used to represent the orbitals) can impact the accuracy of the Hartree-Fock results
    • Larger basis sets (triple-zeta, quadruple-zeta) generally lead to more accurate results but also increase computational cost
    • Basis set incompleteness can introduce errors in the calculated properties, particularly for properties that depend on the electron density far from the nuclei (polarizabilities, dispersion interactions)

Interpreting Hartree-Fock Results

Orbital Energies and Koopmans' Theorem

  • The Hartree-Fock method provides the optimized single-electron wave functions (orbitals) and their corresponding orbital energies
  • The orbital energies can be interpreted as approximate ionization energies according to , which states that the negative of the orbital energy is equal to the ionization energy for removing an electron from that orbital
    • Koopmans' theorem assumes that the orbitals do not relax upon ionization, which is an approximation
  • The shapes and symmetries of the optimized orbitals provide insights into the electronic structure and chemical bonding of the system (σ and π bonds, lone pairs)

Atomic Properties and Post-Hartree-Fock Methods

  • The total Hartree-Fock energy, obtained by summing the orbital energies and correcting for double-counting of electron-electron interactions, serves as an upper bound to the true ground state energy
  • Hartree-Fock calculations can predict various atomic properties, such as electron density distributions, dipole moments, and polarizabilities, which are useful for understanding the behavior and reactivity of atoms and molecules
    • Electron density distributions provide information about the spatial arrangement of electrons and can be used to analyze chemical bonding and intermolecular interactions
    • Dipole moments indicate the separation of charge within a molecule and are important for understanding molecular polarity and reactivity
  • The Hartree-Fock results can serve as a starting point for more accurate post-Hartree-Fock methods that include electron correlation, such as configuration interaction, coupled cluster, or Møller-Plesset perturbation theory (MP2, MP4)
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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.

© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.
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