{"title":"Structural Stability, Thermodynamic and Transport Properties of Indium Under Two-Temperature Heating","authors":"N. A. Smirnov","doi":"10.1002/ctpp.70070","DOIUrl":null,"url":null,"abstract":"<div>\n \n <p>The density functional theory calculations were done to study the structural stability, thermodynamic and transport properties of indium in the two-temperature warm dense matter regime. The calculations show that in the case of “cold” lattice, the increasing electron temperature <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>T</mi>\n <mi>e</mi>\n </msub>\n </mrow>\n <annotation>$$ {T}_e $$</annotation>\n </semantics></math> makes indium gradually change its structure from tetragonal with <span></span><math>\n <semantics>\n <mrow>\n <mi>c</mi>\n <mo>/</mo>\n <mi>a</mi>\n <mo>></mo>\n </mrow>\n <annotation>$$ c/a> $$</annotation>\n </semantics></math> 1 to tetragonal with <span></span><math>\n <semantics>\n <mrow>\n <mi>c</mi>\n <mo>/</mo>\n <mi>a</mi>\n <mo><</mo>\n </mrow>\n <annotation>$$ c/a< $$</annotation>\n </semantics></math> 1 at <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>T</mi>\n <mi>e</mi>\n </msub>\n <mo>></mo>\n </mrow>\n <annotation>$$ {T}_e> $$</annotation>\n </semantics></math> 5.8 kK. One of the intermediate phases in this transformation is the face centered cubic lattice (fcc, <span></span><math>\n <semantics>\n <mrow>\n <mi>c</mi>\n <mo>/</mo>\n <mi>a</mi>\n <mo>=</mo>\n </mrow>\n <annotation>$$ c/a= $$</annotation>\n </semantics></math> 1). Under electron heating the parameter <span></span><math>\n <semantics>\n <mrow>\n <mi>c</mi>\n <mo>/</mo>\n <mi>a</mi>\n </mrow>\n <annotation>$$ c/a $$</annotation>\n </semantics></math> changes smoothly without any discontinuities and the change gets faster as <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>T</mi>\n <mi>e</mi>\n </msub>\n </mrow>\n <annotation>$$ {T}_e $$</annotation>\n </semantics></math> grows. As shown by calculations, the electron–phonon coupling factor of indium is relatively small, <span></span><math>\n <semantics>\n <mrow>\n <mi>G</mi>\n <mo>∼</mo>\n </mrow>\n <annotation>$$ G\\sim $$</annotation>\n </semantics></math> 5 <span></span><math>\n <semantics>\n <mrow>\n <mo>⋅</mo>\n </mrow>\n <annotation>$$ \\cdot $$</annotation>\n </semantics></math> 10<sup>16</sup> W/m<sup>3</sup>/K at 300 K. Its value weakly increases by about 40% as the temperature increases to 10 kK. Additionally, the static electric conductivity and electron thermal conductivity of indium under electron heating to 10<sup>4</sup> K and a finite lattice temperature were calculated through the solution of the Boltzmann transport equation. The paper presents formulas that with good accuracy approximate the calculated dependencies of electric conductivity and thermal conductivity on <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>T</mi>\n <mi>e</mi>\n </msub>\n </mrow>\n <annotation>$$ {T}_e $$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>T</mi>\n <mi>i</mi>\n </msub>\n </mrow>\n <annotation>$$ {T}_i $$</annotation>\n </semantics></math>. It is shown that the known semi-empirical formula for thermal conductivity, <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>κ</mi>\n <mi>e</mi>\n </msub>\n <mo>∼</mo>\n <msub>\n <mi>T</mi>\n <mi>e</mi>\n </msub>\n </mrow>\n <annotation>$$ {\\kappa}_e\\sim {T}_e $$</annotation>\n </semantics></math>/<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>T</mi>\n <mi>i</mi>\n </msub>\n </mrow>\n <annotation>$$ {T}_i $$</annotation>\n </semantics></math>, overestimates <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>κ</mi>\n <mi>e</mi>\n </msub>\n </mrow>\n <annotation>$$ {\\kappa}_e $$</annotation>\n </semantics></math> markedly at <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>T</mi>\n <mi>e</mi>\n </msub>\n <mo>></mo>\n </mrow>\n <annotation>$$ {T}_e> $$</annotation>\n </semantics></math> 2 kK compared to the results obtained in the density functional calculations.</p>\n </div>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"66 7-8","pages":""},"PeriodicalIF":1.1000,"publicationDate":"2026-09-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Contributions to Plasma Physics","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/ctpp.70070","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/12/5 0:00:00","PubModel":"Epub","JCR":"Q3","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
引用次数: 0
Abstract
The density functional theory calculations were done to study the structural stability, thermodynamic and transport properties of indium in the two-temperature warm dense matter regime. The calculations show that in the case of “cold” lattice, the increasing electron temperature makes indium gradually change its structure from tetragonal with 1 to tetragonal with 1 at 5.8 kK. One of the intermediate phases in this transformation is the face centered cubic lattice (fcc, 1). Under electron heating the parameter changes smoothly without any discontinuities and the change gets faster as grows. As shown by calculations, the electron–phonon coupling factor of indium is relatively small, 5 1016 W/m3/K at 300 K. Its value weakly increases by about 40% as the temperature increases to 10 kK. Additionally, the static electric conductivity and electron thermal conductivity of indium under electron heating to 104 K and a finite lattice temperature were calculated through the solution of the Boltzmann transport equation. The paper presents formulas that with good accuracy approximate the calculated dependencies of electric conductivity and thermal conductivity on and . It is shown that the known semi-empirical formula for thermal conductivity, /, overestimates markedly at 2 kK compared to the results obtained in the density functional calculations.
通过密度泛函理论计算,研究了铟在两温温致密物质状态下的结构稳定性、热力学和输运性质。计算表明,在“冷”晶格的情况下,随着电子温度T e $$ {T}_e $$的升高,铟的结构逐渐由与c / a &gt; $$ c/a> $$ 1的四边形转变为与c的四边形/ a &lt; $$ c/a< $$ 1 at T e &gt; $$ {T}_e> $$ 5.8 kK。这种转变的中间相之一是面心立方晶格(fcc, c / a = $$ c/a= $$ 1)。在电子加热条件下,参数c / a $$ c/a $$变化平稳,无间断,且随着T e $$ {T}_e $$的增大,变化速度加快。计算表明,铟的电子-声子耦合系数相对较小,在300 K时为G ~ $$ G\sim $$ 5⋅$$ \cdot $$ 1016 W/m3/K。它的值微弱地增加约40% as the temperature increases to 10 kK. Additionally, the static electric conductivity and electron thermal conductivity of indium under electron heating to 104 K and a finite lattice temperature were calculated through the solution of the Boltzmann transport equation. The paper presents formulas that with good accuracy approximate the calculated dependencies of electric conductivity and thermal conductivity on T e $$ {T}_e $$ and T i $$ {T}_i $$ . It is shown that the known semi-empirical formula for thermal conductivity, κ e ∼ T e $$ {\kappa}_e\sim {T}_e $$ / T i $$ {T}_i $$ , overestimates κ e $$ {\kappa}_e $$ markedly at T e > $$ {T}_e> $$ 2 kK compared to the results obtained in the density functional calculations.