1994
DOI: 10.1103/physrevb.50.2061
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Three-body scattering theory of correlated hole and electron states

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Cited by 39 publications
(28 citation statements)
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“…A detailed comparison between theory and experiment is shown in Figure 6. Figure 7 shows the experimentally extracted imaginary part of the self energy in direct comparison with results based on the DMFT (using a pertrubative FLEX-solver) and an alternative many-body technique, the so called three body scattering (3BS) scheme [81]. A reasonable agreement with the spin-integrated as well as spin-resolved experimental data for all three surfaces and various photon-energies has been achieved.…”
Section: Photoemission Spectroscopysupporting
confidence: 59%
“…A detailed comparison between theory and experiment is shown in Figure 6. Figure 7 shows the experimentally extracted imaginary part of the self energy in direct comparison with results based on the DMFT (using a pertrubative FLEX-solver) and an alternative many-body technique, the so called three body scattering (3BS) scheme [81]. A reasonable agreement with the spin-integrated as well as spin-resolved experimental data for all three surfaces and various photon-energies has been achieved.…”
Section: Photoemission Spectroscopysupporting
confidence: 59%
“…60 The corresponding self-energy DMFT (E) is calculated fully self-consistently (e.g., in charge and selfenergy) from the DMFT. 17,61 Additionally we accounted for correlation effects within the 3BS approximation, 20 where the self-energy is calculated using a configuration interactionlike expansion. Due to the explicit consideration of hole and three-particle configurations this method allows for a detailed analysis of lifetime effects caused by electron-hole pair decays.…”
Section: Theorymentioning
confidence: 99%
“…More recently, theories beyond DFT have been developed to take many-body interaction (i.e., correlation effects) in a more quantitative way into account. In this context we mention the dynamical mean-field theory (DMFT) [17][18][19] which replaces the problem of describing correlation effects in a periodic lattice by a correlated impurity coupled to a self-consistent bath and an alternative approach, the three-body scattering (3BS) approximation 20 which takes into account the relaxation of a hole by an Auger-like excitation in the valence band, formed by one hole plus an electron-hole excitation using a T-matrix formalism. Both theories allow calculating an approximated momentum and energy-dependent spectral function which is described by the bare-particle band structure and the complex self-energy function .…”
Section: Introductionmentioning
confidence: 99%
“…6 On the theoretical side we have calculated spectral functions and quasiparticle energies by solving a multiorbital Hubbard Hamiltonian according to the three-body scattering ͑3BS͒ method. [7][8][9][10][11] This approach can be seen as an extension to the solid state of the configuration-interaction scheme used for finite systems: the Hubbard Hamiltonian is projected on a set of states obtained by adding a finite number of electron-hole pairs to the ground state of the single-particle Hamiltonian and this expansion is truncated to include one electron-hole pair; this approximation is particularly justified for systems with a large band occupation since the role of extra configurations depends on the overall number of empty states necessary for the addition of electron-hole pairs.The effect of electron correlation on one-electron removal energies from a partially filled band is described in terms of interactions between three-body configurations ͑one hole plus one electron-hole pair͒ giving rise to hole-hole and holeelectron scattering; the efficiency of these scattering processes depends first of all on the strength of the screened on-site electron-electron interaction, that is on the Coulomb and exchange integrals U ␣␤ and J ␣␤ : U ␣␤ describes the Coulomb repulsion among opposite spin electrons on the Published in Physical Review B 59 issue 16, R0409-R10412, 1999 which should be used for any reference to this work 1 …”
mentioning
confidence: 99%
“…6 On the theoretical side we have calculated spectral functions and quasiparticle energies by solving a multiorbital Hubbard Hamiltonian according to the three-body scattering ͑3BS͒ method. [7][8][9][10][11] This approach can be seen as an extension to the solid state of the configuration-interaction scheme used for finite systems: the Hubbard Hamiltonian is projected on a set of states obtained by adding a finite number of electron-hole pairs to the ground state of the single-particle Hamiltonian and this expansion is truncated to include one electron-hole pair; this approximation is particularly justified for systems with a large band occupation since the role of extra configurations depends on the overall number of empty states necessary for the addition of electron-hole pairs.…”
mentioning
confidence: 99%