2008
DOI: 10.1007/s00220-008-0664-5
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Analytic Structure of Many-Body Coulombic Wave Functions

Abstract: We investigate the analytic structure of solutions of non-relativistic Schrödinger equations describing Coulombic manyparticle systems. We prove the following: Let ψ(x) with x = (x 1 , . . . , x N ) ∈ R 3N denote an N -electron wavefunction of such a system with one nucleus fixed at the origin. Then in a neighbourhood of a coalescence point, for which x 1 = 0 and the other electron coordinates do not coincide, and differ from 0, ψ can be represented locally as ψ(x) = ψ (1) (x) + |x 1 |ψ (2) (x) with ψ (1) , ψ … Show more

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Cited by 56 publications
(86 citation statements)
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“…However, it has been pointed out by Fournais et al that higher order regularity can be expected for a more general additive ansatz. 13 This is consistent with the early work of Kutzelnigg and Morgen, 14 where, based on such an additive ansatz, different cusp conditions are applied to different types of electron pairs, and thus a higher order convergence (such as M −7/3 ) is achieved. Unfortunately such kind of additive ansatz is not size consistent.…”
Section: Introductionsupporting
confidence: 88%
“…However, it has been pointed out by Fournais et al that higher order regularity can be expected for a more general additive ansatz. 13 This is consistent with the early work of Kutzelnigg and Morgen, 14 where, based on such an additive ansatz, different cusp conditions are applied to different types of electron pairs, and thus a higher order convergence (such as M −7/3 ) is achieved. Unfortunately such kind of additive ansatz is not size consistent.…”
Section: Introductionsupporting
confidence: 88%
“…Our technique of proof can be directly extended to this situation. This observation might be helpful in the approximation of the wave functions in view of their analytic structure outside the coalescence points of more than two particles [5].…”
Section: Introductionmentioning
confidence: 90%
“…This can be deduced without much effort from the results in [5]. The regularizing factor thus covers the singularities of the eigenfunctions in the neighborhood of such points completely.…”
mentioning
confidence: 93%
“…It often serves as a model for electronic wave functions. Its singular behavior at the diagonal x 1 = x 2 is the same as that of the solutions of the electronic Schrödinger equation at the positions where two electrons of distinct spin meet [7]. The function represents at the same time the ground state of the so-called hookium or harmonium atom [11], an artificial two-electron system with the Hamiltonian…”
Section: A Counterexamplementioning
confidence: 87%