Abstract:We deal with the computational determination of the electronic structure and properties of lanthanide ions in complexes and extended structures having open-shell f and d configurations. Particularly, we present conceptual and methodological issues based on Density Functional Theory (DFT) enabling the reliable calculation and description of the f -d transitions in lanthanide doped phosphors. We consider here the optical properties of the Pr 3+ ion embedded into various solid state fluoride host lattices, for th… Show more
“…In cases with more than one electron it cannot be discriminated in the spectral terms from a gap due to the Slater-Condon F 0 (ff) and F 0 (fd) parameters. Thus for the Pr 3+ complexes 19,21 taken as examples in the following, we obtain:…”
Section: Theorymentioning
confidence: 99%
“…[16][17][18][19][20] Therefore, we do not aim in this paper to describe the electrostatic interaction part of the Hamiltonian, i.e. the Slater-Condon parameters relevant for the multi-electron problem, for which our theoretical model has been already improved 19 and revised 21 in previous studies. The calculation of the spin-orbit coupling is placed in the growing efforts devoted nowadays to the relativistic quantum chemistry tools.…”
Section: +mentioning
confidence: 99%
“…21, using the radial functions of the 4f and 5d Kohn-Sham orbitals of Pr 3+ to extract the Slater-Condon parameters. These radial functions are graphically presented in Fig.…”
We discuss the applicability of the Angular Overlap Model (AOM) to evaluate the electronic structure of lanthanide compounds, which are currently the subject of incredible interest in the field of luminescent materials. The functioning of phosphors is well established by the f-d transitions, which requires the investigation of both the ground 4f n and excited 4f nÀ1 5d 1 electron configurations of the lanthanides. The computational approach to the problem is based on the effective Hamiltonian adjusted from ligand field theory, but not restricted to it. The AOM parameterization implies the chemical bonding concept.Focusing our interest on this interaction, we take the advantages offered by modern computational tools to extract AOM parameters, which ensure the transparency of the theoretical determination and convey chemical intuitiveness of the non-empirical results. The given model contributes to the understanding of lanthanides in modern phosphors with high or low site symmetry and presents a non-empirical approach using a less sophisticated computational procedure for the rather complex problem of the ligand field of both 4f and 5d open shells.
“…In cases with more than one electron it cannot be discriminated in the spectral terms from a gap due to the Slater-Condon F 0 (ff) and F 0 (fd) parameters. Thus for the Pr 3+ complexes 19,21 taken as examples in the following, we obtain:…”
Section: Theorymentioning
confidence: 99%
“…[16][17][18][19][20] Therefore, we do not aim in this paper to describe the electrostatic interaction part of the Hamiltonian, i.e. the Slater-Condon parameters relevant for the multi-electron problem, for which our theoretical model has been already improved 19 and revised 21 in previous studies. The calculation of the spin-orbit coupling is placed in the growing efforts devoted nowadays to the relativistic quantum chemistry tools.…”
Section: +mentioning
confidence: 99%
“…21, using the radial functions of the 4f and 5d Kohn-Sham orbitals of Pr 3+ to extract the Slater-Condon parameters. These radial functions are graphically presented in Fig.…”
We discuss the applicability of the Angular Overlap Model (AOM) to evaluate the electronic structure of lanthanide compounds, which are currently the subject of incredible interest in the field of luminescent materials. The functioning of phosphors is well established by the f-d transitions, which requires the investigation of both the ground 4f n and excited 4f nÀ1 5d 1 electron configurations of the lanthanides. The computational approach to the problem is based on the effective Hamiltonian adjusted from ligand field theory, but not restricted to it. The AOM parameterization implies the chemical bonding concept.Focusing our interest on this interaction, we take the advantages offered by modern computational tools to extract AOM parameters, which ensure the transparency of the theoretical determination and convey chemical intuitiveness of the non-empirical results. The given model contributes to the understanding of lanthanides in modern phosphors with high or low site symmetry and presents a non-empirical approach using a less sophisticated computational procedure for the rather complex problem of the ligand field of both 4f and 5d open shells.
“…This is the second calculation route pointed out in the Methodology section. The ZORA Hamiltonian is shown in eqn (13). It results from the zeroth-order regular expansion in e/(2c 2 À V) of the Dirac equation 53 which in general gives very accurate results in atomic calculations, i.e.…”
“…the work of Harry Ramanantoanina et al [23][24][25][26][27][28]), the LFDFT method was extended to handle the electronic structure and properties arising from two-openshell electron configurations for the description of the photophysical properties of lanthanide based phosphors. Presently, the LFDFT is again extended in this work to account for the electronic structure and properties arising from excited three-open-shell electron configurations resulting, in principle, from the excitations of core or semi-core electrons, which are visible in soft or hard regime X-ray absorption fine structure spectroscopy [29][30][31][32][33][34][35] as well as in energy loss spectroscopy [36,37].…”
The ligand field density functional theory (LFDFT) algorithm is extended to treat the electronic structure and properties of systems with three-open-shell electron configurations, exemplified in this work by the calculation of the core and semi-core 1s, 2s, and 3s one-electron excitations in compounds containing transition metal ions. The work presents a model to non-empirically resolve the multiplet energy levels arising from the three-open-shell systems of non-equivalent ns, 3d, and 4p electrons and to calculate the oscillator strengths corresponding to the electric-dipole 3d m → ns 1 3d-m 4p 1 transitions, with n = 1, 2, 3 and m = 0, 1, 2, …, 10 involved in the s electron excitation process. Using the concept of ligand field, the Slater-Condon integrals, the spin-orbit coupling constants, and the parameters of the ligand field potential are determined from density functional theory (DFT). Therefore, a theoretical procedure using LFDFT is established illustrating the spectroscopic details at the atomic scale that can be valuable in the analysis and characterization of the electronic spectra obtained from X-ray absorption fine structure or electron energy loss spectroscopies.
Keywords Ligand field density functional theory (LFDFT) .Three-open-shell electron configuration . Multiplet structure and electric-dipole allowed transitions
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