Hartree–Fock method
E166679
The Hartree–Fock method is an approximate quantum mechanical approach for determining the electronic structure of atoms, molecules, and solids by modeling electrons as occupying self-consistent single-particle orbitals.
All labels observed (9)
| Label | Occurrences |
|---|---|
| Hartree method | 2 |
| Hartree approximation | 1 |
| Hartree-Fock approximation | 1 |
| Hartree–Fock energy | 1 |
| Hartree–Fock method canonical | 1 |
| Roothaan–Hall equations | 1 |
| generalized Hartree–Fock | 1 |
| restricted Hartree–Fock | 1 |
| time-dependent Hartree–Fock | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T1462697 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Hartree–Fock method Context triple: [Pauli exclusion principle, usedIn, Hartree–Fock method]
-
A.
Born–Oppenheimer approximation
The Born–Oppenheimer approximation is a fundamental method in molecular quantum mechanics that simplifies calculations by treating nuclear motion as much slower than electronic motion, allowing their behaviors to be separated.
-
B.
Brillouin–Wigner perturbation theory
Brillouin–Wigner perturbation theory is a formulation of quantum mechanical perturbation theory that uses an energy-dependent effective Hamiltonian to obtain improved approximations to eigenvalues and eigenstates.
-
C.
Herzberg–Teller approximation
The Herzberg–Teller approximation is a refinement in molecular spectroscopy that accounts for vibronic coupling by allowing electronic transition dipole moments to depend on nuclear coordinates, explaining intensity in otherwise forbidden transitions.
-
D.
Rayleigh–Schrödinger perturbation theory
Rayleigh–Schrödinger perturbation theory is a fundamental method in quantum mechanics for approximating the energies and states of a system by treating interactions as small corrections to an exactly solvable problem.
-
E.
Born–Huang expansion
The Born–Huang expansion is a quantum mechanical method that systematically improves upon the Born–Oppenheimer approximation by including couplings between electronic and nuclear motions in molecular systems.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Hartree–Fock method Target entity description: The Hartree–Fock method is an approximate quantum mechanical approach for determining the electronic structure of atoms, molecules, and solids by modeling electrons as occupying self-consistent single-particle orbitals.
-
A.
Born–Oppenheimer approximation
The Born–Oppenheimer approximation is a fundamental method in molecular quantum mechanics that simplifies calculations by treating nuclear motion as much slower than electronic motion, allowing their behaviors to be separated.
-
B.
Brillouin–Wigner perturbation theory
Brillouin–Wigner perturbation theory is a formulation of quantum mechanical perturbation theory that uses an energy-dependent effective Hamiltonian to obtain improved approximations to eigenvalues and eigenstates.
-
C.
Herzberg–Teller approximation
The Herzberg–Teller approximation is a refinement in molecular spectroscopy that accounts for vibronic coupling by allowing electronic transition dipole moments to depend on nuclear coordinates, explaining intensity in otherwise forbidden transitions.
-
D.
Rayleigh–Schrödinger perturbation theory
Rayleigh–Schrödinger perturbation theory is a fundamental method in quantum mechanics for approximating the energies and states of a system by treating interactions as small corrections to an exactly solvable problem.
-
E.
Born–Huang expansion
The Born–Huang expansion is a quantum mechanical method that systematically improves upon the Born–Oppenheimer approximation by including couplings between electronic and nuclear motions in molecular systems.
- F. None of above. chosen
Statements (59)
| Predicate | Object |
|---|---|
| instanceOf |
ab initio method
ⓘ
approximate quantum mechanical method ⓘ electronic structure method ⓘ mean-field approximation ⓘ quantum chemistry method ⓘ |
| accountsFor | exchange interaction ⓘ |
| appliesTo |
atoms
ⓘ
molecules ⓘ solids ⓘ |
| approximates | many-electron wavefunction ⓘ |
| assumes | independent-particle model ⓘ |
| basedOn | Schrödinger equation ⓘ |
| computationalScaling | approximately O(N^4) with system size ⓘ |
| developedBy |
Douglas Hartree
ⓘ
Vladimir Fock ⓘ |
| enforces | Pauli exclusion principle ⓘ |
| field |
computational chemistry
ⓘ
condensed matter physics ⓘ quantum chemistry ⓘ |
| hasVariant |
Hartree–Fock method
self-linksurface differs
ⓘ
surface form:
generalized Hartree–Fock
multiconfigurational Hartree–Fock ⓘ relativistic Hartree–Fock ⓘ Hartree–Fock method self-linksurface differs ⓘ
surface form:
restricted Hartree–Fock
restricted open-shell Hartree–Fock ⓘ Hartree–Fock method self-linksurface differs ⓘ
surface form:
time-dependent Hartree–Fock
unrestricted Hartree–Fock ⓘ |
| historicalPrecursor |
Hartree–Fock method
self-linksurface differs
ⓘ
surface form:
Hartree method
|
| improvesUpon |
Hartree–Fock method
self-linksurface differs
ⓘ
surface form:
Hartree method
|
| input |
basis set
ⓘ
nuclear charges ⓘ nuclear coordinates ⓘ |
| neglects | dynamic electron correlation ⓘ |
| output |
electron density
ⓘ
molecular orbital coefficients ⓘ total electronic energy ⓘ |
| relatedTo | density functional theory ⓘ |
| solvedBy |
Hartree–Fock method
self-linksurface differs
ⓘ
surface form:
Roothaan–Hall equations
self-consistent field procedure ⓘ |
| solvesFor |
molecular orbitals
ⓘ
orbital energies ⓘ total electronic energy ⓘ |
| typicalImplementation |
Gaussian-type orbital basis sets
ⓘ
Slater-type orbital basis sets ⓘ |
| usedAsReferenceFor |
Møller–Plesset perturbation theory
ⓘ
configuration interaction ⓘ coupled-cluster theory ⓘ post-Hartree–Fock methods ⓘ |
| usedFor |
ground-state electronic structure calculations
ⓘ
molecular property calculations ⓘ potential energy surface generation ⓘ |
| usesApproximation |
Born–Oppenheimer approximation
ⓘ
mean-field approximation ⓘ |
| usesConcept |
Slater determinant
ⓘ
antisymmetry of fermionic wavefunctions ⓘ self-consistent field ⓘ single-particle orbitals ⓘ |
| yields |
Fock matrix
ⓘ
Fock operator ⓘ Hartree–Fock method self-linksurface differs ⓘ
surface form:
Hartree–Fock energy
|
How these facts were elicited
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Subject: Hartree–Fock method Description of subject: The Hartree–Fock method is an approximate quantum mechanical approach for determining the electronic structure of atoms, molecules, and solids by modeling electrons as occupying self-consistent single-particle orbitals.
Referenced by (10)
Full triples — surface form annotated when it differs from this entity's canonical label.