A DFT study to explore structural, elastic, mechanical, phonon, electronic and optical properties of halide perovskites AgXF 3 ( X = Be , Ca ) $$ {\mathrm{AgXF}}_3\left(\mathrm{X}=\mathrm{Be},\mathrm{Ca}\right) $$ with PBEsol, TB-mBJ and SCAN functionals

IF 2.3 3区 化学 Q3 CHEMISTRY, PHYSICAL
H. Bushra Munir, A. Afaq, Abdelaziz Gassoumi, Muhammad Ahmed, Abu Bakar
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Afaq,&nbsp;Abdelaziz Gassoumi,&nbsp;Muhammad Ahmed,&nbsp;Abu Bakar","doi":"10.1002/qua.27447","DOIUrl":null,"url":null,"abstract":"<p>First principles calculations have been performed using full potential linearized augmented plane wave, FP-LAPW, within Wien2k to elucidate structural, elastic, mechanical, phonon, electronic and optical properties of lead free halide perovskites <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>AgXF</mtext>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n <mo>(</mo>\n <mi>X</mi>\n <mo>=</mo>\n <mi>Be</mi>\n <mo>,</mo>\n <mi>Ca</mi>\n <mo>)</mo>\n </mrow>\n <annotation>$$ {\\mathrm{AgXF}}_3\\left(\\mathrm{X}=\\mathrm{Be},\\mathrm{Ca}\\right) $$</annotation>\n </semantics></math>. The energy volume curve fitting is used to examine structural stability. For structural optimization and mechanical properties, we employed Perdew–Burke–Ernzerhof generalized gradient approximation and PBEsol, revised for solids, exchange and correlation functional. The optimized lattice constant of <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>AgBeF</mtext>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{AgBeF}}_3 $$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>AgCaF</mtext>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{AgCaF}}_3 $$</annotation>\n </semantics></math> is 3.631 and 4.349Å. The elastic constant <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>C</mtext>\n </mrow>\n <mrow>\n <mn>11</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{C}}_{11} $$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>C</mtext>\n </mrow>\n <mrow>\n <mn>12</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{C}}_{12} $$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>C</mtext>\n </mrow>\n <mrow>\n <mn>44</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{C}}_{44} $$</annotation>\n </semantics></math> are computed to extract different mechanical parameters like Poisson's ratio, Pugh's ratio, bulk modulus, shear modulus, Young's modulus, anisotropic ratio, Cauchy pressure and shear constant. The mechanical parameters exhibit greater structural, mechanical and dynamical stability of <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>AgBeF</mtext>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{AgBeF}}_3 $$</annotation>\n </semantics></math> than <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>AgCaF</mtext>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{AgCaF}}_3 $$</annotation>\n </semantics></math>. The electronic and optical properties are calculated by using TB-mBJ and SCAN potentials in addition to PBEsol. The electronic band gap of <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>AgBeF</mtext>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{AgBeF}}_3 $$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mrow>\n <mtext>AgCaF</mtext>\n </mrow>\n <mrow>\n <mn>3</mn>\n </mrow>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{AgCaF}}_3 $$</annotation>\n </semantics></math> is 4.71 and 6.01 eV with TB-mBJ and both perovskites are indirect band gap materials. The optical response of these perovskites against wide range of incident electromagnetic radiation is assessed by calculating absorption, reflection, optical conductivity, dielectric constant, energy loss function and refraction. 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引用次数: 0

Abstract

First principles calculations have been performed using full potential linearized augmented plane wave, FP-LAPW, within Wien2k to elucidate structural, elastic, mechanical, phonon, electronic and optical properties of lead free halide perovskites AgXF 3 ( X = Be , Ca ) $$ {\mathrm{AgXF}}_3\left(\mathrm{X}=\mathrm{Be},\mathrm{Ca}\right) $$ . The energy volume curve fitting is used to examine structural stability. For structural optimization and mechanical properties, we employed Perdew–Burke–Ernzerhof generalized gradient approximation and PBEsol, revised for solids, exchange and correlation functional. The optimized lattice constant of AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ and AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ is 3.631 and 4.349Å. The elastic constant C 11 $$ {\mathrm{C}}_{11} $$ , C 12 $$ {\mathrm{C}}_{12} $$ and C 44 $$ {\mathrm{C}}_{44} $$ are computed to extract different mechanical parameters like Poisson's ratio, Pugh's ratio, bulk modulus, shear modulus, Young's modulus, anisotropic ratio, Cauchy pressure and shear constant. The mechanical parameters exhibit greater structural, mechanical and dynamical stability of AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ than AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ . The electronic and optical properties are calculated by using TB-mBJ and SCAN potentials in addition to PBEsol. The electronic band gap of AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ and AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ is 4.71 and 6.01 eV with TB-mBJ and both perovskites are indirect band gap materials. The optical response of these perovskites against wide range of incident electromagnetic radiation is assessed by calculating absorption, reflection, optical conductivity, dielectric constant, energy loss function and refraction. Strong absorption, high optical conductivity and low reflectivity indicates that AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ and AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ are promising materials for photovoltaic applications.

利用 PBEsol、TB-mBJ 和 SCAN 函数进行 DFT 研究,探索卤化物包晶 AgXF 3 ( X = Be , Ca ) $$ {\mathrm{AgXF}}_3\left(\mathrm{X}=\mathrm{Be},\mathrm{Ca}\right) $$ 的结构、弹性、机械、声子、电子和光学特性
在 Wien2k 中使用全电势线性化增强平面波(FP-LAPW)进行了第一性原理计算,以阐明无铅卤化物包晶 AgXF 3 ( X = Be , Ca ) $$ {\mathrm{AgXF}}_3\left(\mathrm{X}=\mathrm{Be},\mathrm{Ca}\right) $$ 的结构、弹性、机械、声子、电子和光学特性。能量体积曲线拟合用于检验结构稳定性。在结构优化和力学性能方面,我们采用了 Perdew-Burke-Ernzerhof 广义梯度近似和 PBEsol,并对固体、交换和相关函数进行了修正。AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ 和 AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ 的优化晶格常数分别为 3.631 和 4.349 Å。弹性常数 C 11 $${\mathrm{C}}_{11}$$ , C 12 $$ {\mathrm{C}}_{12}$$ 和 C 44 $$ {\mathrm{C}}_{44}$$ 计算得出不同的力学参数,如泊松比、普氏比、体积模量、剪切模量、杨氏模量、各向异性比、考希压力和剪切常数。力学参数显示 AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ 比 AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ 具有更高的结构、力学和动力学稳定性。除了 PBEsol 之外,还使用 TB-mBJ 和 SCAN 电位计算了电子和光学性质。通过 TB-mBJ 计算,AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ 和 AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ 的电子带隙分别为 4.71 和 6.01 eV,这两种包晶石都是间接带隙材料。通过计算吸收、反射、光导率、介电常数、能量损失函数和折射率,评估了这些包晶对各种入射电磁辐射的光学响应。强烈的吸收、高光导率和低反射率表明 AgBeF 3 $$ {\mathrm{AgBeF}}_3 $$ 和 AgCaF 3 $$ {\mathrm{AgCaF}}_3 $$ 是很有前途的光伏应用材料。
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来源期刊
International Journal of Quantum Chemistry
International Journal of Quantum Chemistry 化学-数学跨学科应用
CiteScore
4.70
自引率
4.50%
发文量
185
审稿时长
2 months
期刊介绍: Since its first formulation quantum chemistry has provided the conceptual and terminological framework necessary to understand atoms, molecules and the condensed matter. Over the past decades synergistic advances in the methodological developments, software and hardware have transformed quantum chemistry in a truly interdisciplinary science that has expanded beyond its traditional core of molecular sciences to fields as diverse as chemistry and catalysis, biophysics, nanotechnology and material science.
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