Ab inilio CI c;llcul.lwd sTTecls 01 elecmon corrclakn on high-energ) electron scaIwring LTOFF ascrions arc prrsun~cd ror "son logelher with a relawd polenkd ensrgy analysts or the correlaCon energy. The thcorericnl rcrul~ mcludmg sllrnaws 01 the full correlation clfecls. arc In good agreemen! wth ex
Electron correlation and the compton profile of atomic neon
โ Scribed by Vedene H. Smith Jr.; Richard Edwin Brown
- Publisher
- Elsevier Science
- Year
- 1973
- Tongue
- English
- Weight
- 450 KB
- Volume
- 20
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
โฆ Synopsis
The radial momentum distribution lo(p) and the Compton profile Jc(l!) are determined for atomic neon from several restricted Hartrec-Fock (RHF) wavefunctions and two configuration interaction (CI) wavefunctions. The CI functions are the we!l correlated (fulI "second-order") function of Viers, Schaeffer and Harris, and the Ahlrichs-Hinze multi-configuration Hartree-Fock (MCHF) function which include:; only L-shell correlation. It is found for this completely closed shell system thai the effects of electron correlation are quite small. This contrasts with the .resuIts for systems such as Be( 'S) and B('P) where the semi-internal and internal correlation effects were responsible for significant discrepancies between the RHF and CI results. These results indicate that n wavefunction which carefully includes the semi-internal, orbital polarization, and internal correlations beyond the RHF wavefunction (i.e., a "Brst-order" or "chage$ensity" function), should account for the principal correlation effects on the Compton profiles and momentum distributions.
๐ SIMILAR VOLUMES
The wcond-order energy for Ne is computed starting with the symmetric sum of oneclectron Hartree-Fock operators as the Teroth-ordcr hamiltonian. The variational-perturbation pair functions of dcfmite orbital and spin symmetry are expressed in the form of partial wave expansions. Special attention is
Electron energy-loss spectra. obtamrd for Ne and Ar, are analysed tn terms of Compton profiles (CPs). The euperimental CPs do not peak at q = 0, nor are they symmetrtcal as to theu maxImum value, as predlcted withm the framework of the lmpulsc approuunatlon. Thus Yompton defect" IS charactertsed by