Investigations on the EPR g factors and local structures for the orthorhombic and tetragonal Cu2+ centers in Pb[Zr0.54Ti0.46]O3

The defect models of the orthorhombical and tetragonal Cu2+ centers in Pb[Zr0.54Ti0.46]O3 are attributed to Cu2+ ions occupying the sixfold coordinated octahedral Ti4+ site with and without charge compensation, respectively. The electron paramagnetic resonance (EPR) g factors gi (i = x, y, z) of the...

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Veröffentlicht in:Magnetic resonance in chemistry 2024-10, Vol.62 (10), p.732-739
Hauptverfasser: Huang, Xiaohua, Zhang, Meiyun, Guo, Fangfang, Cai, Houdao, Zhou, Xilin, Feng, Cuidi
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container_title Magnetic resonance in chemistry
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creator Huang, Xiaohua
Zhang, Meiyun
Guo, Fangfang
Cai, Houdao
Zhou, Xilin
Feng, Cuidi
description The defect models of the orthorhombical and tetragonal Cu2+ centers in Pb[Zr0.54Ti0.46]O3 are attributed to Cu2+ ions occupying the sixfold coordinated octahedral Ti4+ site with and without charge compensation, respectively. The electron paramagnetic resonance (EPR) g factors gi (i = x, y, z) of the Cu2+ centers in Pb[Zr0.54Ti0.46]O3 are theoretically studied by using the perturbation formulas of a 3d9 ion under orthorhombically and tetragonally elongated octahedra. Based on the calculation, the impurity off‐center displacements are about 0.253 and 0.162 Å for the orthorhombical and tetragonal Cu2+ centers, respectively. Meanwhile, the planar Cu2+–O2− bonds are found to experience the relative variation ΔR (≈0.102 Å) along the a‐ and b‐axes for the orthorhombical Cu2+ center due to the Jahn–Teller (JT) effect. The theoretical EPR g factors based on the above local structures agree well with the observed values. Local structure of Cu2+ centers (site 1 and site 2) in Pb[Zr0.54Ti0.46]O3. Local structure of Cu2+ center with one oxygen vacancies (VO) along the C4‐axis (site 1). Local structure of Cu2+ center with [CuO6]10− cluster without charge compensation (site 2).
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The electron paramagnetic resonance (EPR) g factors gi (i = x, y, z) of the Cu2+ centers in Pb[Zr0.54Ti0.46]O3 are theoretically studied by using the perturbation formulas of a 3d9 ion under orthorhombically and tetragonally elongated octahedra. Based on the calculation, the impurity off‐center displacements are about 0.253 and 0.162 Å for the orthorhombical and tetragonal Cu2+ centers, respectively. Meanwhile, the planar Cu2+–O2− bonds are found to experience the relative variation ΔR (≈0.102 Å) along the a‐ and b‐axes for the orthorhombical Cu2+ center due to the Jahn–Teller (JT) effect. The theoretical EPR g factors based on the above local structures agree well with the observed values. Local structure of Cu2+ centers (site 1 and site 2) in Pb[Zr0.54Ti0.46]O3. Local structure of Cu2+ center with one oxygen vacancies (VO) along the C4‐axis (site 1). 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The electron paramagnetic resonance (EPR) g factors gi (i = x, y, z) of the Cu2+ centers in Pb[Zr0.54Ti0.46]O3 are theoretically studied by using the perturbation formulas of a 3d9 ion under orthorhombically and tetragonally elongated octahedra. Based on the calculation, the impurity off‐center displacements are about 0.253 and 0.162 Å for the orthorhombical and tetragonal Cu2+ centers, respectively. Meanwhile, the planar Cu2+–O2− bonds are found to experience the relative variation ΔR (≈0.102 Å) along the a‐ and b‐axes for the orthorhombical Cu2+ center due to the Jahn–Teller (JT) effect. The theoretical EPR g factors based on the above local structures agree well with the observed values. Local structure of Cu2+ centers (site 1 and site 2) in Pb[Zr0.54Ti0.46]O3. Local structure of Cu2+ center with one oxygen vacancies (VO) along the C4‐axis (site 1). Local structure of Cu2+ center with [CuO6]10− cluster without charge compensation (site 2).</abstract><doi>10.1002/mrc.5472</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0003-0760-3464</orcidid></addata></record>
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electron paramagnetic resonance
local structures
Pb[Zr0.54Ti0.46]O3
title Investigations on the EPR g factors and local structures for the orthorhombic and tetragonal Cu2+ centers in Pb[Zr0.54Ti0.46]O3
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