New High-Pressure Polymorphs of Rb2CO3 and Cs2CO3: Crystal Structure Prediction and P–T Phase Diagrams

IF 4.8 3区 化学 Q2 CHEMISTRY, MULTIDISCIPLINARY
Anastassiya V. Mezentseva, Nursultan E. Sagatov, Dinara N. Sagatova, Maksim V. Banaev, Pavel N. Gavryushkin
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Gavryushkin","doi":"10.1002/jcc.70363","DOIUrl":null,"url":null,"abstract":"<div>\n \n <p>In this work, we performed crystal structure searches for rubidium and cesium carbonates (Rb<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math> and Cs<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math>) in the pressure range of 0–100 GPa using evolutionary algorithms based on the density functional theory. As a result, two new stable high-pressure polymorphs, <span></span><math>\n <semantics>\n <mrow>\n <mi>C</mi>\n <mi>c</mi>\n </mrow>\n <annotation>$$ Cc $$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <mi>C</mi>\n <mn>2</mn>\n <mo>/</mo>\n <mi>c</mi>\n </mrow>\n <annotation>$$ C2/c $$</annotation>\n </semantics></math>, were predicted for both carbonates. The M<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math>-<span></span><math>\n <semantics>\n <mrow>\n <mi>C</mi>\n <mn>2</mn>\n <mo>/</mo>\n <mi>c</mi>\n </mrow>\n <annotation>$$ C2/c $$</annotation>\n </semantics></math> (M = Rb, Cs) phase is isostructural with the high-pressure K<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math>-<span></span><math>\n <semantics>\n <mrow>\n <mi>C</mi>\n <mn>2</mn>\n <mo>/</mo>\n <mi>c</mi>\n </mrow>\n <annotation>$$ C2/c $$</annotation>\n </semantics></math> phase, whereas the M<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math>-<span></span><math>\n <semantics>\n <mrow>\n <mi>C</mi>\n <mi>c</mi>\n </mrow>\n <annotation>$$ Cc $$</annotation>\n </semantics></math> phase has no known structural analogs and represents a novel phase for alkali metal carbonates. A common sequence of phase transitions was established for both compounds: <span></span><math>\n <semantics>\n <mrow>\n <mi>P</mi>\n <msub>\n <mrow>\n <mn>2</mn>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msub>\n <mo>/</mo>\n <mi>c</mi>\n </mrow>\n <annotation>$$ P{2}_1/c $$</annotation>\n </semantics></math> <span></span><math>\n <semantics>\n <mrow>\n <mo>↔</mo>\n </mrow>\n <annotation>$$ \\leftrightarrow $$</annotation>\n </semantics></math> <span></span><math>\n <semantics>\n <mrow>\n <mi>C</mi>\n <mi>c</mi>\n </mrow>\n <annotation>$$ Cc $$</annotation>\n </semantics></math> <span></span><math>\n <semantics>\n <mrow>\n <mo>↔</mo>\n </mrow>\n <annotation>$$ \\leftrightarrow $$</annotation>\n </semantics></math> <span></span><math>\n <semantics>\n <mrow>\n <mi>C</mi>\n <mn>2</mn>\n <mo>/</mo>\n <mi>c</mi>\n </mrow>\n <annotation>$$ C2/c $$</annotation>\n </semantics></math>. For Rb<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math>, the transition pressures are 4.9 GPa and 23.4 GPa, and for Cs<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math>, they are 5.2 GPa and 35.5 GPa. The phonon calculations confirmed the dynamic stability of all predicted phases. It was also shown that these high-pressure phases cannot be quenched to ambient pressure. Within the quasi-harmonic approximation, <i>P–T</i> phase diagrams of Rb<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math> and Cs<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>CO<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_3 $$</annotation>\n </semantics></math> were constructed for the first time, revealing a weak temperature dependence of the phase boundaries. The obtained results elucidate a general trend in the phase transitions of alkali metal carbonates: under high pressure, the cation sublattices of all alkali carbonates tend to adopt an AlB<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow></mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {}_2 $$</annotation>\n </semantics></math>-type configuration, with the transition pressure increasing systematically with the ionic radius of the cation.</p>\n </div>","PeriodicalId":188,"journal":{"name":"Journal of Computational Chemistry","volume":"47 9","pages":""},"PeriodicalIF":4.8000,"publicationDate":"2026-04-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Computational Chemistry","FirstCategoryId":"92","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/jcc.70363","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0

Abstract

In this work, we performed crystal structure searches for rubidium and cesium carbonates (Rb 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ and Cs 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ ) in the pressure range of 0–100 GPa using evolutionary algorithms based on the density functional theory. As a result, two new stable high-pressure polymorphs, C c $$ Cc $$ and C 2 / c $$ C2/c $$ , were predicted for both carbonates. The M 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ - C 2 / c $$ C2/c $$ (M = Rb, Cs) phase is isostructural with the high-pressure K 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ - C 2 / c $$ C2/c $$ phase, whereas the M 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ - C c $$ Cc $$ phase has no known structural analogs and represents a novel phase for alkali metal carbonates. A common sequence of phase transitions was established for both compounds: P 2 1 / c $$ P{2}_1/c $$ $$ \leftrightarrow $$ C c $$ Cc $$ $$ \leftrightarrow $$ C 2 / c $$ C2/c $$ . For Rb 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ , the transition pressures are 4.9 GPa and 23.4 GPa, and for Cs 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ , they are 5.2 GPa and 35.5 GPa. The phonon calculations confirmed the dynamic stability of all predicted phases. It was also shown that these high-pressure phases cannot be quenched to ambient pressure. Within the quasi-harmonic approximation, P–T phase diagrams of Rb 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ and Cs 2 $$ {}_2 $$ CO 3 $$ {}_3 $$ were constructed for the first time, revealing a weak temperature dependence of the phase boundaries. The obtained results elucidate a general trend in the phase transitions of alkali metal carbonates: under high pressure, the cation sublattices of all alkali carbonates tend to adopt an AlB 2 $$ {}_2 $$ -type configuration, with the transition pressure increasing systematically with the ionic radius of the cation.

Rb2CO3和Cs2CO3新的高压晶型:晶体结构预测和P-T相图。
在这项工作中,我们使用基于密度泛函理论的进化算法在0-100 GPa的压力范围内对铷和铯碳酸盐(Rb 2 $$ {}_2 $$ CO 3 $$ {}_3 $$和Cs 2 $$ {}_2 $$ CO 3 $$ {}_3 $$)进行了晶体结构搜索。结果表明,两种碳酸盐均有两种新的稳定高压晶型,C - C $$ Cc $$和C - 2 / C $$ C2/c $$。2m $$ {}_2 $$ CO 3 $$ {}_3 $$ - c2 / C $$ C2/c $$ (M = Rb, Cs)相与高压k2 $$ {}_2 $$ CO 3 $$ {}_3 $$ - c2 / C $$ C2/c $$相具有相同的结构,而2m $$ {}_2 $$ CO 3 $$ {}_3 $$ - C $$ Cc $$相没有已知的结构类似物,代表了碱金属碳酸盐的一种新相。两个化合物建立了一个共同的相变序列:p1 / c $$ P{2}_1/c $$↔$$ \leftrightarrow $$ c c $$ Cc $$↔$$ \leftrightarrow $$ c2 / c $$ C2/c $$。Rb 2 $$ {}_2 $$ CO 3 $$ {}_3 $$的转化压力分别为4.9 GPa和23.4 GPa, Cs 2 $$ {}_2 $$ CO 3 $$ {}_3 $$的转化压力分别为5.2 GPa和35.5 GPa。声子计算证实了所有预测相的动态稳定性。研究还表明,这些高压相不能被淬火到环境压力。在准谐波近似下,首次构建了Rb 2 $$ {}_2 $$ CO 3 $$ {}_3 $$和Cs 2 $$ {}_2 $$ CO 3 $$ {}_3 $$的P-T相图,揭示了相界对温度的弱依赖性。所得结果阐明了碱金属碳酸盐相变的总体趋势:在高压下,所有碱金属碳酸盐的阳离子亚晶格都倾向于采用alb2 $$ {}_2 $$型构型,且转变压力随着阳离子离子半径的增大而系统地增大。
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来源期刊
CiteScore
6.60
自引率
3.30%
发文量
247
审稿时长
1.7 months
期刊介绍: This distinguished journal publishes articles concerned with all aspects of computational chemistry: analytical, biological, inorganic, organic, physical, and materials. The Journal of Computational Chemistry presents original research, contemporary developments in theory and methodology, and state-of-the-art applications. Computational areas that are featured in the journal include ab initio and semiempirical quantum mechanics, density functional theory, molecular mechanics, molecular dynamics, statistical mechanics, cheminformatics, biomolecular structure prediction, molecular design, and bioinformatics.
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