2016
DOI: 10.1021/acs.jctc.6b00376
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Efficient Computation of the Hartree–Fock Exchange in Real-Space with Projection Operators

Abstract: We describe an efficient projection-based real-space implementation of the nonlocal single-determinant exchange operator. Through a matrix representation of the projected operator, we show that this scheme works equally well for both occupied and virtual states. Our scheme reaches a speedup of 2 orders of magnitude and has no significant loss of accuracy compared to an implementation of the full nonlocal single-determinant exchange operator. We find excellent agreement upon comparing Hartree-Fock eigenvalues, … Show more

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Cited by 25 publications
(26 citation statements)
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“…For performing hybrid functional calculations, we implement the Fock operator in DARSEC using the self-consistent scheme described in Ref. [63]. We note that efficient projection approximations for the Fock exchange operator are given Refs.…”
Section: B Exact Remainder Potentialsmentioning
confidence: 99%
“…For performing hybrid functional calculations, we implement the Fock operator in DARSEC using the self-consistent scheme described in Ref. [63]. We note that efficient projection approximations for the Fock exchange operator are given Refs.…”
Section: B Exact Remainder Potentialsmentioning
confidence: 99%
“…For performing hybrid functional calculations, we have implemented the Fock operator in DARSEC using the self-consistent scheme described in ref. [60]. We note that efficient projection approximations for the Fock exchange operator have been given [60][61][62][63], but for the small systems studied here use of the full (unprojected) Fock operator was found to be sufficient.…”
Section: B Exact Remainder Potentialsmentioning
confidence: 87%
“…In contrast, the exact HF exchange interaction is nonlocal; however, it can be truncated to finite range in large systems, especially if exact exchange is only included within a short range, as in the popular Heyd‐Scuseria‐Ernzerhof functional . Alternatively, the evaluation of exact exchange can be sped up with projection operators; or the Krieger‐Li‐Iafrate (KLI) approximation can be used to build a fully local exchange potential, also allowing exact‐exchange calculations on large systems . Further necessary steps in the implementation of large‐scale real‐space approaches involve replacing the full matrix diagonalization in the conventional Roothaan orbital update of Equation with an iterative approach such as the Davidson method that is used to solve only for the new occupied subspace, or avoiding diagonalization altogether by using, for example, Green's function methods to solve for the new occupied orbitals, as in the Helmholtz kernel method …”
Section: Applicationsmentioning
confidence: 99%