Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physics Letters B

Time-dependent Hartree-Fock phase: Unique implication of variational principle

Peter C. Lichtner, James J. Griffin, Hildegard Schultheis, Rainer Schultheis, Anatole B. Volkov

Published Dec 1, 1979• 15 citations
Publisher
DOI
10.1016/0370-2693(79)90452-0

Related papers

Derivation of an adiabatic time-dependent Hartree-Fock formalism from a variational principle

D.M. Brink, M.J. Giannoni, M. Vénéroni

Nuclear Physics A•Feb 1, 1976•113 citations

Variational derivation of the adiabatic time-dependent Hartree--Fock formalism

D.M. Brink, M.J. Giannoni, M. Vénéroni +2 more

•Jan 1, 1975•0 citations

Variational derivation of a time-dependent Hartree-Fock Hamiltonian

Peter C. Lichtner, James J. Griffin, Hildegard Schultheis +2 more

The variational derivation of the time-dependent Hartree-Fock equation is reviewed. When norm-violating variations are included, a unique time-dependent Hartree-Fock Hamiltonian, which differs from that customarily used in time-dependent Hartree-Fock analyses, is implied. This variationally "true" Hartree-Fock Hamiltonian has the same expectation value as the exact Hamiltonian, equal to the average energy of the system. Since this quantity remains constant under time-dependent Hartree-Fock time evolution, we suggest the label "constant $〈H〉$" for this form of time-dependent Hartree-Fock theory.NUCLEAR REACTIONS Unique time-dependent Hartree-Fock Hamiltonian obtained from variational principle by norm-violating variations.

Physical Review C•Aug 1, 1979•7 citations

Time-Dependent Hartree-Fock and its Extension

正俊 山村, 惇 栗山

素粒子論研究•Jul 20, 1984•0 citations

Time-dependent hartree-fock method and its extension

日本物理学会, 京都大学基礎物理学研究所, 正俊 山村 +1 more

•Jan 1, 1987•1 citation

Generalized variational principle for the time-dependent Hartree-Fock equations for a Slater determinant

Hans-Jörg Kull, Dieter Pfirsch

The time-dependent Hartree-Fock equations are derived from a variational principle for the general N-body action of a Slater determinant of single-electron orbitals. The variational principle generalizes commonly used variational treatments based on reduced two-body actions. The self-consistent field equations are found to contain time-dependent corrections to the standard mean-field interactions. Their physical significance is discussed and a time-dependent phase shift to the Slater determinant is obtained that properly accounts for the total interaction energy in the mean-field approach.

Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics•May 1, 2000•19 citations
The variational derivation of the time-dependent Hartree-Fock equation is reviewed. When norm-violating variations are included, a unique time-dependent Hartree-Fock Hamiltonian, which differs from that customarily used in time-dependent Hartree-Fock analyses, is implied. This variationally "true" Hartree-Fock Hamiltonian has the same expectation value as the exact Hamiltonian, equal to the average energy of the system. Since this quantity remains constant under time-dependent Hartree-Fock time evolution, we suggest the label "constant 〈H〉〈H〉〈H〉" for this form of time-dependent Hartree-Fock theory.NUCLEAR REACTIONS Unique time-dependent Hartree-Fock Hamiltonian obtained from variational principle by norm-violating variations.
The time-dependent Hartree-Fock equations are derived from a variational principle for the general N-body action of a Slater determinant of single-electron orbitals. The variational principle generalizes commonly used variational treatments based on reduced two-body actions. The self-consistent field equations are found to contain time-dependent corrections to the standard mean-field interactions. Their physical significance is discussed and a time-dependent phase shift to the Slater determinant is obtained that properly accounts for the total interaction energy in the mean-field approach.