Internal Electric Fields and Structural Instabilities in Insulating Transition Metal Compounds: Influence on Optical Properties

Abstract This work reviews new ideas developed in the last two decades which play a key role for understanding the optical properties of insulating materials containing transition metal (TM) cations. Initially, this review deals with compounds involving d 4 and d 9 ions where the local structure of the involved MX 6 complexes (M=d n cation, X=ligand) is never cubic but distorted, a fact widely ascribed to the Jahn‐Teller (JT) effect. Nevertheless, that assumption is often wrong as the JT coupling requires an orbitally degenerate ground state in the initial geometry a condition not fulfilled even if the lattice is tetragonal. For this reason, the equilibrium geometry of d 4 and d 9 complexes in low symmetry lattices, is influenced by two factors: (i) The effects, usually ignored, of the internal electric field, E R , due to the rest of lattice ions on the active electrons localized in the MX 6 unit. (ii) The existence of structural instabilities driven by vibronic interactions that lead to negative force constants. As first examples of these ideas, we show that the equilibrium structure, electronic ground state of KZnF 3 :Cu 2+ , K 2 ZnF 4 :Cu 2+ and K 2 CuF 4 obey to different causes and only in KZnF 3 :Cu 2+ the JT effect takes place. These ideas also explain the local structure and optical properties of CuF 2 , CrF 2 or KAlCuF 6 compounds where the JT effect is symmetry forbidden and those of layered copper chloroperovskites where the orthorhombic instability explains the red shift of one d−d transition under pressure. In a second step, this review explores stable systems involving d 3 , d 5 or d 9 cations, where the internal electric field, E R , is responsible for some puzzling phenomena. This is the case of ruby and emerald that surprisingly exhibit a different color despite the Cr 3+ ‐O 2− distance is the same. A similar situation holds when comparing the normal (KMgF 3 ) and the inverted (LiBaF 3 ) perovskites doped with Mn 2+ having the same Mn 2+ ‐F distance but clearly different optical spectra. The role of E R is particularly remarkable looking for the origin of the color in the historical Egyptian Blue pigment based on CaCuSi 4 O 10 .

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Journal
ChemPhotoChem
Published
2024-08-13
DOI
https://doi.org/10.1002/cptc.202400024
Citations
1
Primary Topic
ZnO doping and properties
Type
article
Field-Weighted Citation Impact
0.12
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article

Internal Electric Fields and Structural Instabilities in Insulating Transition Metal Compounds: Influence on Optical Properties

J. M. Garcı́a-Lastra, Pablo García‐Fernández, J. A. Aramburu, Inés Sánchez‐Movellán et al.
1 citations
ChemPhotoChem
ZnO doping and properties
0.12
article

Internal Electric Fields and Structural Instabilities in Insulating Transition Metal Compounds: Influence on Optical Properties

J. M. Garcı́a-Lastra, Pablo García‐Fernández, J. A. Aramburu, Inés Sánchez‐Movellán, M. Moreno
article en
1 citations

Abstract

Abstract This work reviews new ideas developed in the last two decades which play a key role for understanding the optical properties of insulating materials containing transition metal (TM) cations. Initially, this review deals with compounds involving d 4 and d 9 ions where the local structure of the involved MX 6 complexes (M=d n cation, X=ligand) is never cubic but distorted, a fact widely ascribed to the Jahn‐Teller (JT) effect. Nevertheless, that assumption is often wrong as the JT coupling requires an orbitally degenerate ground state in the initial geometry a condition not fulfilled even if the lattice is tetragonal. For this reason, the equilibrium geometry of d 4 and d 9 complexes in low symmetry lattices, is influenced by two factors: (i) The effects, usually ignored, of the internal electric field, E R , due to the rest of lattice ions on the active electrons localized in the MX 6 unit. (ii) The existence of structural instabilities driven by vibronic interactions that lead to negative force constants. As first examples of these ideas, we show that the equilibrium structure, electronic ground state of KZnF 3 :Cu 2+ , K 2 ZnF 4 :Cu 2+ and K 2 CuF 4 obey to different causes and only in KZnF 3 :Cu 2+ the JT effect takes place. These ideas also explain the local structure and optical properties of CuF 2 , CrF 2 or KAlCuF 6 compounds where the JT effect is symmetry forbidden and those of layered copper chloroperovskites where the orthorhombic instability explains the red shift of one d−d transition under pressure. In a second step, this review explores stable systems involving d 3 , d 5 or d 9 cations, where the internal electric field, E R , is responsible for some puzzling phenomena. This is the case of ruby and emerald that surprisingly exhibit a different color despite the Cr 3+ ‐O 2− distance is the same. A similar situation holds when comparing the normal (KMgF 3 ) and the inverted (LiBaF 3 ) perovskites doped with Mn 2+ having the same Mn 2+ ‐F distance but clearly different optical spectra. The role of E R is particularly remarkable looking for the origin of the color in the historical Egyptian Blue pigment based on CaCuSi 4 O 10 .

ChemPhotoChemVol. 8(12)
Universidad de Cantabria (ES), Technical University of Denmark (DK)
Sustainable cities and communities
Openalex Percentile: Top 61%
ZnO doping and properties
0.12
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