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Hartree–Fock method

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Hartree–Fock method
NameHartree–Fock method
ClassificationAb initio quantum chemistry methods
Founded yearc. 1930
Key peopleDouglas Hartree, Vladimir Fock, John C. Slater
Related methodsPost-Hartree–Fock methods, Density functional theory

Hartree–Fock method. The Hartree–Fock method is a foundational Self-consistent field approach in Computational chemistry and Quantum chemistry for approximating the Wave function and Energy of a quantum many-body system. It provides the starting point for most Ab initio quantum chemistry methods by solving the Schrödinger equation for molecules and atoms under the mean-field approximation. The method is named for the pioneering work of Douglas Hartree and its later generalization by Vladimir Fock.

Overview

The central goal of the Hartree–Fock method is to determine the best single Slater determinant approximation to the Ground state of a system of electrons moving in the field of atomic nuclei. It is a cornerstone of Theoretical chemistry, forming the basis for more accurate Post-Hartree–Fock methods like Coupled cluster and Configuration interaction. The method's output, the Hartree–Fock limit, represents the optimal energy achievable within its theoretical constraints. Its development was significantly advanced by the work of Clemens C. J. Roothaan and George G. Hall, who formulated the algebraic equations for practical computations on digital computers.

Theoretical foundation

The method is derived from the Variational principle, seeking the Slater determinant that minimizes the total electronic energy of the system defined by the Molecular Hamiltonian. The key simplification is the replacement of the complex electron-electron interactions with an average effective potential, leading to the Fock operator. This operator acts on one-electron functions called molecular orbitals, which are solutions to the Hartree–Fock equation. The theoretical formulation for closed-shell systems is often attributed to John C. Slater, while the open-shell generalization is credited to Vladimir Fock. The equations are typically solved within the Linear combination of atomic orbitals approximation, as formalized by Clemens C. J. Roothaan.

Algorithm and implementation

A standard Hartree–Fock calculation is an iterative Self-consistent field procedure. It begins with an initial guess for the molecular orbitals, often from a simpler method like Hückel theory or a Semi-empirical quantum chemistry method. The algorithm then constructs the Fock matrix using integrals over the basis set, such as those developed in the GAUSSIAN program. The matrix is diagonalized to obtain new orbitals and a new Density matrix, a cycle repeated until convergence in the total energy is achieved. Major software packages implementing the method include GAUSSIAN, GAMESS, NWChem, and PSI4. The method for periodic systems is implemented in codes like VASP and CRYSTAL.

Limitations and extensions

The primary limitation of the Hartree–Fock method is its neglect of dynamic electron correlation, as it treats electrons as moving in an average field. This leads to systematic errors, such as overestimation of bond energies and failure to describe dispersion interactions. To address these shortcomings, a hierarchy of Post-Hartree–Fock methods has been developed, including Møller–Plesset perturbation theory (particularly MP2), Configuration interaction (e.g., CISD), and Coupled cluster (e.g., CCSD(T)). An alternative framework that incorporates correlation from the outset is Density functional theory, pioneered by Walter Kohn and Pierre Hohenberg.

Applications

Despite its limitations, the Hartree–Fock method remains widely used for calculating equilibrium geometries, harmonic frequencies, and dipole moments for a vast array of molecules, from small systems like water to larger organic compounds. It serves as the essential reference wavefunction for more advanced Ab initio quantum chemistry methods in studies of chemical reaction pathways and spectroscopic properties. The method is also foundational in developing molecular mechanics force fields and is employed in materials science for investigating electronic structures of solids within the periodic Hartree–Fock framework. Category:Computational chemistry Category:Quantum chemistry Category:Ab initio quantum chemistry methods