{"title":"First-Principles Molecular Dynamics Study of M<sub>3</sub>AlF<sub>6</sub> (M= Li/Na/K) Molten Salts.","authors":"Wendi Zhang, Xianwei Hu, Hongguang Kang, Ruidong Guo, Jiangyu Yu, Zhaowen Wang","doi":"10.1021/acs.jpcb.4c07043","DOIUrl":null,"url":null,"abstract":"<p><p>The microscopic properties and Raman spectra of molten, Li<sub>3</sub>AlF<sub>6</sub>, Na<sub>3</sub>AlF<sub>6</sub>, and K<sub>3</sub>AlF<sub>6</sub> systems were investigated using first-principles molecular dynamics combined with the Voronoi tessellation method. The results have indicated that Li<sup>+</sup>, Na<sup>+</sup>, and K<sup>+</sup> exist in a free state, whereas Al<sup>3+</sup> and F<sup>-</sup> form ion clusters ([AlF<sub><i>x</i></sub>]<sup>3</sup><sup>-</sup><i><sup>x</sup></i>) with evidence of free F<sup>-</sup> anions. The nature of the alkali metal cation does not significantly affect the average Al-F bond length (1.775 Å). The coordination numbers of Al<sup>3+</sup> and F<sup>-</sup> are 5.22, 5.21, and 4.95 in Li<sub>3</sub>AlF<sub>6</sub>, Na<sub>3</sub>AlF<sub>6</sub> and K<sub>3</sub>AlF<sub>6</sub>, respectively, indicating a lower content of [AlF<sub>6</sub>]<sup>3-</sup> and [AlF<sub>5</sub>]<sup>2-</sup> in K<sub>3</sub>AlF<sub>6</sub>. The self-diffusion coefficients decrease in the order Li<sup>+</sup> > Na<sup>+</sup> > K<sup>+</sup>, and the trend is Na<sub>3</sub>AlF<sub>6</sub> > Li<sub>3</sub>AlF<sub>6</sub> > K<sub>3</sub>AlF<sub>6</sub> for Al<sup>3+</sup> and F<sup>-</sup>. The alkali metal cation has little effect on changes in the atomic charge and spin population of Al<sup>3+</sup>. Single bonds form between Al<sup>3+</sup> and F<sup>-</sup> and exhibit uneven bond order. The upper limits of the HOMO-LUMO gaps for Li<sub>3</sub>AlF<sub>6</sub>, Na<sub>3</sub>AlF<sub>6</sub> and K<sub>3</sub>AlF<sub>6</sub> are, 4.82, 2.10, and 3.51 eV, respectively, suggesting higher conductivity of Na<sub>3</sub>AlF<sub>6</sub> relative to Li<sub>3</sub>AlF<sub>6</sub> and K<sub>3</sub>AlF<sub>6</sub> under superheating conditions (40 K above the liquidus temperature).</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":" ","pages":""},"PeriodicalIF":2.8000,"publicationDate":"2025-02-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Journal of Physical Chemistry B","FirstCategoryId":"1","ListUrlMain":"https://doi.org/10.1021/acs.jpcb.4c07043","RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
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Abstract
The microscopic properties and Raman spectra of molten, Li3AlF6, Na3AlF6, and K3AlF6 systems were investigated using first-principles molecular dynamics combined with the Voronoi tessellation method. The results have indicated that Li+, Na+, and K+ exist in a free state, whereas Al3+ and F- form ion clusters ([AlFx]3-x) with evidence of free F- anions. The nature of the alkali metal cation does not significantly affect the average Al-F bond length (1.775 Å). The coordination numbers of Al3+ and F- are 5.22, 5.21, and 4.95 in Li3AlF6, Na3AlF6 and K3AlF6, respectively, indicating a lower content of [AlF6]3- and [AlF5]2- in K3AlF6. The self-diffusion coefficients decrease in the order Li+ > Na+ > K+, and the trend is Na3AlF6 > Li3AlF6 > K3AlF6 for Al3+ and F-. The alkali metal cation has little effect on changes in the atomic charge and spin population of Al3+. Single bonds form between Al3+ and F- and exhibit uneven bond order. The upper limits of the HOMO-LUMO gaps for Li3AlF6, Na3AlF6 and K3AlF6 are, 4.82, 2.10, and 3.51 eV, respectively, suggesting higher conductivity of Na3AlF6 relative to Li3AlF6 and K3AlF6 under superheating conditions (40 K above the liquidus temperature).
期刊介绍:
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