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Electron Densities from Gas‐Phase Electron Diffraction Intensities. II. Molecular Hartree–Fock Cross Sections

dc.contributor.authorKohl, D. A.en_US
dc.contributor.authorBartell, Lawrence S.en_US
dc.date.accessioned2010-05-06T21:41:20Z
dc.date.available2010-05-06T21:41:20Z
dc.date.issued1969-10-01en_US
dc.identifier.citationKohl, D. A.; Bartell, L. S. (1969). "Electron Densities from Gas‐Phase Electron Diffraction Intensities. II. Molecular Hartree–Fock Cross Sections." The Journal of Chemical Physics 51(7): 2896-2904. <http://hdl.handle.net/2027.42/70136>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70136
dc.description.abstractDifferential cross sections for electron scattering based on molecular Hartree–Fock electron densities are compared with cross sections based on the independent‐atom approximation for the molecules C2, N2, O2, F2, and CO. The results show that bonding effects on the electron density manifest themselves to the extent of several percent in the scattered intensity at small scattering angles. Furthermore, molecule‐to‐molecule variations in the shifts of electron density are clearly reflected in variations in the functional form of the scattered intensity. A comparison of the calculated intensities for N2 and O2 with preliminary experimental intensities suggests that electron scattering techniques now in development should be able to provide information about bonding and electron correlation effects competitive in accuracy with that of current quantum‐mechanical calculations.en_US
dc.format.extent3102 bytes
dc.format.extent580800 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleElectron Densities from Gas‐Phase Electron Diffraction Intensities. II. Molecular Hartree–Fock Cross Sectionsen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Chemistry and Institute of Science and Technology, The University of Michigan, Ann Arbor, Michigan 48104en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70136/2/JCPSA6-51-7-2896-1.pdf
dc.identifier.doi10.1063/1.1672430en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
dc.identifier.citedreferenceD. A. Kohl and L. S. Bartell, J. Chem. Phys. 51, 2891 (1969), Paper I.en_US
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dc.identifier.citedreferenceT. G. Strand, D. A. Kohl, and R. A. Bonham, J. Chem. Phys. 39, 1307 (1963).en_US
dc.identifier.citedreferenceL. S. Bartell and R. M. Gavin, Jr., J. Am. Chem. Soc. 86, 3493 (1964); J. Chem. Phys. 43, 856 (1965); R. M. Gavin, Jr. and L. S. Bartell, 44, 3687 (1966); 45, 4700 (1966).en_US
dc.identifier.citedreferenceD. A. Kohl and R. A. Bonham, J. Chem. Phys. 47, 1634 (1967).en_US
dc.identifier.citedreferenceM. Abramowitz and I. A. Stegun, Handbook of Mathematical Functions (U.S. Government Printing Office, Washington, D.C., 1965), Eq. 10.1.47, p. 440.en_US
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dc.owningcollnamePhysics, Department of


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