Single-photon double ionization: renormalized-natural-orbital theory versus multi-configurational Hartree–Fock. (20th June 2017)

• Record Type: Journal Article
• Authors: Brics, M; Rapp, J; Bauer, D
• Is Part Of: Journal of physics. Volume 50:Number 14(2017:Jul. 15)
• Publication Date: 2017-06-20
• Subjects: single-photon double ionization -- correlated photoelectron spectra -- density matrices -- time-dependent density functional theory -- multi-configurational time-dependent Hartree–Fock; 32.80.Fb -- 31.15.ee -- 31.70.Hq -- 02.70.-c; Atoms -- Periodicals; Molecules -- Periodicals; Optics -- Periodicals; Nuclear physics -- Periodicals; 539.6
• DOI: 10.1088/1361-6455/aa7585
• Languages: English
• ISSNs: 0953-4075

Abstract

Abstract: The N -particle wavefunction has too many dimensions for a direct time propagation of a many-body system according to the time-dependent Schrödinger equation (TDSE). On the other hand, time-dependent density functional theory (TDDFT) tells us that the single-particle density is, in principle, sufficient. However, a practicable equation of motion for the accurate time evolution of the single-particle density is unknown. It is thus an obvious idea to propagate a quantity which is not as reduced as the single-particle density but less dimensional than the N -body wavefunction. Recently, we have introduced time-dependent renormalized-natural-orbital theory (TDRNOT). TDRNOT is based on the propagation of the eigenfunctions of the one-body reduced density matrix, the so-called natural orbitals. In this paper we demonstrate how TDRNOT is related to the multi-configurational time-dependent Hartree–Fock (MCTDHF) approach. We also compare the performance of MCTDHF and TDRNOT versus the TDSE for single-photon double ionization (SPDI) of a 1D helium model atom. SPDI is one of the effects where TDDFT does not work in practice, especially if one is interested in correlated photoelectron spectra, for which no explicit density functional is known.