“…The recently developed strongly constrained and appropriately normed (SCAN) meta-GGA functional 1 has demonstrated a superior performance in reproducing the fundamental physical properties and phenomena associated with correlated oxides. [2][3][4][5][6][7][8] Furthermore, studies have shown that incorporating the SCAN functional into the DFT+U framework (SCAN+U) can enhance the accuracy in reproducing certain physical properties of transition metal oxides. [9][10][11][12][13] For example, Carter and coworkers demonstrated that the introduction of the Hubbard term improves the reproduction of the ground-state properties of binary 3d TM oxides, being critical for the prediction of the most stable polymorphs of Mn 2 O 3 and Fe 3 O 4 .…”
“…The recently developed strongly constrained and appropriately normed (SCAN) meta-GGA functional 1 has demonstrated a superior performance in reproducing the fundamental physical properties and phenomena associated with correlated oxides. [2][3][4][5][6][7][8] Furthermore, studies have shown that incorporating the SCAN functional into the DFT+U framework (SCAN+U) can enhance the accuracy in reproducing certain physical properties of transition metal oxides. [9][10][11][12][13] For example, Carter and coworkers demonstrated that the introduction of the Hubbard term improves the reproduction of the ground-state properties of binary 3d TM oxides, being critical for the prediction of the most stable polymorphs of Mn 2 O 3 and Fe 3 O 4 .…”
“…Since the development of DFT by Holenberg, Kohn, and Sham, , a great deal of improvement on exchange-correlation (XC) functionals has been reported, such as the widely used generalized gradient approximation (GGA) developed in the late 1980s. , The GGA functionals have offered some acceptable results in the modeling of perovskite oxides based on d 0 transition metals (TM). − However, the overestimation of electron delocalization and metallic character is a known failure of DFT methods for systems with localized and strongly interacting d -electrons and f -electrons. − In the 1990s, the DFT + U method introduced an explicit treatment of electron correlation with a Hubbard-like model for a subset of states in the system. , Vast literature demonstrates the suitability of the DFT + U approach to investigate TM oxides with strong Coulomb correlations. More recently, the strongly constrained and appropriately normed (SCAN) meta-GGA functional has shown good performance to model the basic physical properties and phenomena associated to correlated oxides. , For instance, investigations on perovskite-related oxides using meta-GGA functionals (and particularly SCAN) have accurately described the transition from the insulating to the metallic character of La 2 CuO 4 by substitution of La by Sr in the superconducting system; the layered ordering stabilization of the Bi 2 MFeO 6 perovskites (M = Al, Ga, In) induced by the Fe–magnetic interactions; the effect of the hole and electron doping in the electronic structure of Sm 1– x M x NiO 3 (M = Ca, Ce); and have predicted the structural cubic-symmetry breaking, band-gap existence, and magnetic behavior in ABO 3 perovskites with B = 3 d -TM …”
Section: Introductionmentioning
confidence: 99%
“…More recently, the strongly constrained and appropriately normed (SCAN) meta-GGA functional 15 has shown good performance to model the basic physical properties and phenomena associated to correlated oxides. 16 , 17 For instance, investigations on perovskite-related oxides using meta-GGA functionals (and particularly SCAN) have accurately described the transition from the insulating to the metallic character of La 2 CuO 4 by substitution of La by Sr in the superconducting system; 18 the layered ordering stabilization of the Bi 2 MFeO 6 perovskites (M = Al, Ga, In) induced by the Fe–magnetic interactions; 19 the effect of the hole and electron doping in the electronic structure of Sm 1– x M x NiO 3 (M = Ca, Ce); 20 and have predicted the structural cubic-symmetry breaking, band-gap existence, and magnetic behavior in ABO 3 perovskites with B = 3 d -TM. 21 …”
Progress in the design of functional perovskite oxides relies on advances in density functional theory (DFT) methods to efficiently and effectively model complex systems composed of several transition-metal ions. This work reports the application of DFT methods to investigate the electronic structure of the YSr 2 Cu 2 FeO 8−δ (0 < δ < 1) family in which the insulating, metal, or superconducting behaviors and even anion conductivity can be tuned by modifying the oxygen content. In particular, we assess the performance of the generalized gradient approximation (GGA), its Hubbard-U correction (GGA + U), and the strongly constrained and appropriately normed (SCAN) to model the metallic (idealized YSr 2 Cu 2 FeO 8 ) and insulating (idealized YSr 2 Cu 2 FeO 7 ) phases of the system. The analysis of the DFT results is supported by DC resistivity measurements that denote the metal character of the synthesized YSr 2 Cu 2 FeO 7.86 and the semiconducting character of YSr 2 Cu 2 FeO 7.08 prepared under reducing conditions. In addition, the band gap of YSr 2 Cu 2 FeO 7.08 , in the range of 0.73−1.2 eV, has been extracted from diffuse reflectance spectroscopy (DRS). While the three methodologies (GGA, GGA + U, SCAN) permit the reproduction of the crystal structures of the synthetized oxides (determined here in the case of YSr 2 Cu 2 FeO 7.08 by neutron powder diffraction (NPD)), the SCAN emerges as the only one capable to predict the basic electronic and magnetic properties across the YSr 2 Cu 2 FeO 8−δ (0 < δ < 1) series. The picture that emerges for the metal (δ = 0) to insulating (δ = 1) transition is the one in which oxygen vacancies contribute electrons to the filling of the Cu/Fe-3d x 2 −y 2 states of the conduction band. These results validate the SCAN functional for future DFT investigations of complex functional oxides that combine several transition metals.
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