Analysis of electron interaction and atomic shell structure in terms of local potentials

The Kohn–Sham potential vs of an N‐electron system and the potential veff of the Euler–Lagrange equation for the square root of the electron density are expressed as the sum of the external potential plus potentials related to the electronic structure, such as the potential of the electron Coulomb repulsion, including the Hartree potential and the screening due to exchange and correlation, a potential representing the effect of Fermi–Dirac statistics and Coulomb correlation on the kinetic functional, and additional potentials representing ‘‘response’’ effects on these potentials. For atoms several of these potentials have distinct atomic shell structure: One of them has peaks between the shells, while two others are step functions. In one of those step functions the steps represent characteristic shell energies. Examples of the potentials extracted from the optimized potential model (OPM) are presented for Kr and Cd. Correlation potentials, obtained by subtracting the exchange potential of the OPM from (n...

[1]  G. Hunter The exact one-electron model of molecular structure , 1986 .

[2]  Baerends,et al.  Analysis of correlation in terms of exact local potentials: Applications to two-electron systems. , 1989, Physical review. A, General physics.

[3]  B. Deb,et al.  New method for the direct calculation of electron density in many‐electron systems. I. Application to closed‐shell atoms , 1983 .

[4]  P. Acharya,et al.  On the functional derivative of the kinetic energy density functional , 1982 .

[5]  Á. Nagy Analysis of the Pauli potential of atoms and ions , 1991 .

[6]  A. Bunge,et al.  Accurate electron density and one‐electron properties for the beryllium atom , 1987 .

[7]  W. Kohn,et al.  Self-Consistent Equations Including Exchange and Correlation Effects , 1965 .

[8]  David N. Beratan,et al.  Localized orbitals and the Fermi hole , 1982 .

[9]  Parr,et al.  Construction of exact Kohn-Sham orbitals from a given electron density. , 1993, Physical review. A, Atomic, molecular, and optical physics.

[10]  Robert G. Parr,et al.  Quantities T sub s ( n ) and T sub c ( n ) in density-functional theory , 1992 .

[11]  Lévy,et al.  Exact properties of the Pauli potential for the square root of the electron density and the kinetic energy functional. , 1988, Physical review. A, General physics.

[12]  M. Levy Universal variational functionals of electron densities, first-order density matrices, and natural spin-orbitals and solution of the v-representability problem. , 1979, Proceedings of the National Academy of Sciences of the United States of America.

[13]  N. H. March The local potential determining the square root of the ground-state electron density of atoms and molecules from the Schrödinger equation , 1986 .

[14]  J. D. Talman,et al.  Optimized central potentials for atomic ground-state wavefunctions , 1978 .

[15]  R. Daudel,et al.  The Electron Pair in Chemistry , 1974 .

[16]  W. A. Bingel The Behaviour of the First-Order Density Matrix at the Coulomb Singularities of the Schrödinger Equation , 1963 .

[17]  Stott,et al.  Effective potentials in density-functional theory. , 1988, Physical review. B, Condensed matter.

[18]  March,et al.  Construction of the Pauli potential, Pauli energy, and effective potential from the electron density. , 1991, Physical review. A, Atomic, molecular, and optical physics.

[19]  J. D. Talman,et al.  Optimized effective atomic central potential , 1976 .

[20]  J. C. Slater A Simplification of the Hartree-Fock Method , 1951 .

[21]  R. Leeuwen,et al.  Exchange-correlation potential with correct asymptotic behavior. , 1994, Physical review. A, Atomic, molecular, and optical physics.

[22]  R. Dreizler,et al.  Density Functional Theory: An Approach to the Quantum Many-Body Problem , 1991 .