FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2013807722> ?p ?o ?g. }

• W2013807722 endingPage "93" @default.
• W2013807722 startingPage "81" @default.
• W2013807722 abstract "A general method of obtaining accurate and useful many-electron wave functions for atoms and molecules is developed. The method involves the proper optimization of a many-electron function which is an eigen-function of total spin and which satisfies Pauli's principle. The procedure is somewhat similar to that in which one obtains the Hartree-Fock wave function by properly optimizing a Slater determinant. There are three key features of the new method: (1) The wave function remains accurate as the nuclei configuration is changed from the equilibrium configuration to that of the dissociated molecule; (2) the many-electron wave function can be interpreted in an independent-particle scheme; (3) the independent-particle states are no longer always required to be symmetry functions for the spatial symmetry group as in the Hartree-Fock method. In addition, the energy calculated using the new method is always lower than the Hartree-Fock energy, and the method is applicable to states of any total spin and number of particles. Calculations using this method are reported for the ${mathrm{H}}_{2}$ and LiH molecules." @default.
• W2013807722 created "2016-06-24" @default.
• W2013807722 creator A5035627473 @default.
• W2013807722 date "1967-05-05" @default.
• W2013807722 modified "2023-10-14" @default.
• W2013807722 title "Improved Quantum Theory of Many-Electron Systems. II. The Basic Method" @default.
• W2013807722 cites W135867663 @default.
• W2013807722 cites W1644384521 @default.
• W2013807722 cites W1966020783 @default.
• W2013807722 cites W1966996977 @default.
• W2013807722 cites W1974955349 @default.
• W2013807722 cites W1980438315 @default.
• W2013807722 cites W1981363283 @default.
• W2013807722 cites W1982568518 @default.
• W2013807722 cites W1985900077 @default.
• W2013807722 cites W1989486778 @default.
• W2013807722 cites W1993967022 @default.
• W2013807722 cites W1995696119 @default.
• W2013807722 cites W2011079470 @default.
• W2013807722 cites W2014209007 @default.
• W2013807722 cites W2016342922 @default.
• W2013807722 cites W2032077419 @default.
• W2013807722 cites W2035028578 @default.
• W2013807722 cites W2038167210 @default.
• W2013807722 cites W2042876294 @default.
• W2013807722 cites W2054314146 @default.
• W2013807722 cites W2057882530 @default.
• W2013807722 cites W2057936594 @default.
• W2013807722 cites W2067600085 @default.
• W2013807722 cites W2070711817 @default.
• W2013807722 cites W2074530207 @default.
• W2013807722 cites W2077394341 @default.
• W2013807722 cites W2083456180 @default.
• W2013807722 cites W2086904202 @default.
• W2013807722 cites W2090765455 @default.
• W2013807722 cites W2090789410 @default.
• W2013807722 cites W2111866034 @default.
• W2013807722 cites W2140684507 @default.
• W2013807722 cites W2156397715 @default.
• W2013807722 cites W2170095176 @default.
• W2013807722 cites W3038453665 @default.
• W2013807722 doi "https://doi.org/10.1103/physrev.157.81" @default.
• W2013807722 hasPublicationYear "1967" @default.
• W2013807722 type Work @default.
• W2013807722 sameAs 2013807722 @default.
• W2013807722 citedByCount "244" @default.
• W2013807722 countsByYear W20138077222012 @default.
• W2013807722 countsByYear W20138077222013 @default.
• W2013807722 countsByYear W20138077222014 @default.
• W2013807722 countsByYear W20138077222015 @default.
• W2013807722 countsByYear W20138077222016 @default.
• W2013807722 countsByYear W20138077222017 @default.
• W2013807722 countsByYear W20138077222018 @default.
• W2013807722 countsByYear W20138077222019 @default.
• W2013807722 countsByYear W20138077222020 @default.
• W2013807722 countsByYear W20138077222021 @default.
• W2013807722 countsByYear W20138077222022 @default.
• W2013807722 countsByYear W20138077222023 @default.
• W2013807722 crossrefType "journal-article" @default.
• W2013807722 hasAuthorship W2013807722A5035627473 @default.
• W2013807722 hasBestOaLocation W20138077222 @default.
• W2013807722 hasConcept C110340908 @default.
• W2013807722 hasConcept C113603373 @default.
• W2013807722 hasConcept C113630233 @default.
• W2013807722 hasConcept C121332964 @default.
• W2013807722 hasConcept C14036430 @default.
• W2013807722 hasConcept C147120987 @default.
• W2013807722 hasConcept C174038435 @default.
• W2013807722 hasConcept C184779094 @default.
• W2013807722 hasConcept C189394030 @default.
• W2013807722 hasConcept C2524010 @default.
• W2013807722 hasConcept C2779886137 @default.
• W2013807722 hasConcept C33923547 @default.
• W2013807722 hasConcept C42704618 @default.
• W2013807722 hasConcept C62520636 @default.
• W2013807722 hasConcept C78458016 @default.
• W2013807722 hasConcept C86803240 @default.
• W2013807722 hasConcept C86966772 @default.
• W2013807722 hasConcept C97355855 @default.
• W2013807722 hasConceptScore W2013807722C110340908 @default.
• W2013807722 hasConceptScore W2013807722C113603373 @default.
• W2013807722 hasConceptScore W2013807722C113630233 @default.
• W2013807722 hasConceptScore W2013807722C121332964 @default.
• W2013807722 hasConceptScore W2013807722C14036430 @default.
• W2013807722 hasConceptScore W2013807722C147120987 @default.
• W2013807722 hasConceptScore W2013807722C174038435 @default.
• W2013807722 hasConceptScore W2013807722C184779094 @default.
• W2013807722 hasConceptScore W2013807722C189394030 @default.
• W2013807722 hasConceptScore W2013807722C2524010 @default.
• W2013807722 hasConceptScore W2013807722C2779886137 @default.
• W2013807722 hasConceptScore W2013807722C33923547 @default.
• W2013807722 hasConceptScore W2013807722C42704618 @default.
• W2013807722 hasConceptScore W2013807722C62520636 @default.
• W2013807722 hasConceptScore W2013807722C78458016 @default.
• W2013807722 hasConceptScore W2013807722C86803240 @default.
• W2013807722 hasConceptScore W2013807722C86966772 @default.
• W2013807722 hasConceptScore W2013807722C97355855 @default.
• W2013807722 hasIssue "1" @default.

• next