“…It has been pointed out that the GTOs do not have a correct behaviour for large p-values while the STOs do [3]. On the other hand in the regions of interest in momentum space the use of GTO functions is satisfactory [28].…”
This review is primarily concerned with theoretical calculations of momentum densities and Compton cross sections for molecular systems. Qualitative properties of a momentum space representation are given. A comparison between experimental and theoretical cross sections within the impulse approximation is made. Ab initio calculations for small molecules, like the nitrogen and water molecules, are studied. Various approaches to treat large molecules are studied and compared for the formamide and p-benzoquinone molecules. Some comments on calculations for solid state systems are given.
“…It has been pointed out that the GTOs do not have a correct behaviour for large p-values while the STOs do [3]. On the other hand in the regions of interest in momentum space the use of GTO functions is satisfactory [28].…”
This review is primarily concerned with theoretical calculations of momentum densities and Compton cross sections for molecular systems. Qualitative properties of a momentum space representation are given. A comparison between experimental and theoretical cross sections within the impulse approximation is made. Ab initio calculations for small molecules, like the nitrogen and water molecules, are studied. Various approaches to treat large molecules are studied and compared for the formamide and p-benzoquinone molecules. Some comments on calculations for solid state systems are given.
“…Similar formulae are written for G , and G, which correspond toy and z components, respectively. In Equation (2 1) , the summations over I, J a n d K are done under the restriction I + J + K = Y.The G function defined by Equation(22) has been abbreviated as Gp'(m, n I x).…”
(42) and (43) and on page 378, the superscripts ( q ) on the H and H functions should be deleted. (43)
5) In EquationOn page 375, line 9 from bottom, lb + lb + rn, + n, should read la + lb + rn, + n,.
The effect of basis functions on molecular one-electron property expectation values calculated by approximate methods is examined using weighted and unweighted least-squares Gaussian-type orbital function expansions of Slater-type orbital functions.
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