Solving Staticand Dynamic Disorder in Cu<sub>4</sub>TiTe<sub>4</sub>: Crystal Structureand Thermodynamic Properties

Cu<sub>4</sub>TiTe<sub>4</sub> shows positional disorder because one of the copper atoms does not occupy a precise position in the unit cell. This fact complicates the development of simple and reliable crystalline models capable of capturing the promising thermodynamic and optical properties of Cu<sub>4</sub>TiTe<sub>4</sub>. Here, we select practical supercells accounting for the different Cu atomic environments in the crystal and identify nonequivalent structural configurations. Their electronic energies and thermodynamic properties are calculated by coupling DFT and the quasi-harmonic approximations. Average values corresponding to the experimentally observed Cu<sub>4</sub>TiTe<sub>4</sub> structure are obtained introducing Boltzmann weights based on the total energy of these configurations. For Cu<sub>4</sub>TiTe<sub>4</sub>, differences in the calculated properties among the 16 nonequivalent configurations of its 2 × 2 × 1 supercell demonstrate the inadequacy of focusing just on a single configuration. After calculating the energy barriers associated with the diffusion of the disordered copper atoms among its four equivalent positions (lower than 0.5 eV), we evidence the importance of taking into account this dynamic disorder, which reveals a negative thermal expansion for this telluride at low temperatures, not found under the static disorder approach.

Publication Details

Journal
Figshare
Published
2025-02-07
DOI
https://doi.org/10.1021/acs.inorgchem.4c04585.s001
Primary Topic
Mycorrhizal Fungi and Plant Interactions
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article
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article

Solving Staticand Dynamic Disorder in Cu4TiTe4: Crystal Structureand Thermodynamic Properties

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Mycorrhizal Fungi and Plant Interactions
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Solving Staticand Dynamic Disorder in Cu4TiTe4: Crystal Structureand Thermodynamic Properties

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Abstract

Cu<sub>4</sub>TiTe<sub>4</sub> shows positional disorder because one of the copper atoms does not occupy a precise position in the unit cell. This fact complicates the development of simple and reliable crystalline models capable of capturing the promising thermodynamic and optical properties of Cu<sub>4</sub>TiTe<sub>4</sub>. Here, we select practical supercells accounting for the different Cu atomic environments in the crystal and identify nonequivalent structural configurations. Their electronic energies and thermodynamic properties are calculated by coupling DFT and the quasi-harmonic approximations. Average values corresponding to the experimentally observed Cu<sub>4</sub>TiTe<sub>4</sub> structure are obtained introducing Boltzmann weights based on the total energy of these configurations. For Cu<sub>4</sub>TiTe<sub>4</sub>, differences in the calculated properties among the 16 nonequivalent configurations of its 2 × 2 × 1 supercell demonstrate the inadequacy of focusing just on a single configuration. After calculating the energy barriers associated with the diffusion of the disordered copper atoms among its four equivalent positions (lower than 0.5 eV), we evidence the importance of taking into account this dynamic disorder, which reveals a negative thermal expansion for this telluride at low temperatures, not found under the static disorder approach.

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Solving Staticand Dynamic Disorder in Cu<sub>4</sub>TiTe<sub>4</sub>: Crystal Structureand Thermodynamic Properties · Figshare (2025) | TGRS Research Map | TGRS