{"title":"电流材料特性的改变,由多潘兰坦宁方法的二分之一浓度变化所改变","authors":"Wisanggeni Bayu Aji, H. Sutrisno","doi":"10.20961/alchemy.18.1.53333.80-94","DOIUrl":null,"url":null,"abstract":"<p>Energi celah pita dan <em>density of state</em> (DOS) dari NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0; 0,25; 0,50 dan 0,75) dapat diprediksi secara teoritis menggunakan pendekatan <em>density functional theory</em> (DFT). Perhitungan awal berdasarkan atas pendekatan <em>local density approximation</em> (LDA) dan <em>generalized gradient approximation</em> dari Perdew-Burke-Ernzerhof (GGA+PBE) sebagai fungsional tukar-korelasi. Perhitungan awal energi celah pita dan DOS dilakukan pada unit sel konvensional (1×1×1) untuk NaYTiO<sub>4</sub> dan supersel (2×2×1) untuk NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0,25; 0,50 dan 0,75) dengan program CASTEP Materials Studio. Hasil perhitungan menunjukkan energi celah pita (<em>E<sub>g</sub></em>) sebesar 3,447; 3,384; 3,356 dan 3,560 eV untuk x = 0; 0,25; 0,50 dan 0,75 dengan metode LDA. Di sisi lain, metode GGA+PBE menunjukkan <em>E<sub>g</sub> </em>sebesar 3,039; 2,963 dan 2,930 eV untuk x = 0; 0,25; 0,50 dan 0,75. Hasil perhitungan karakter DOS menunjukkan bahwa seluruh material menunjukkan transisi <em>E<sub>g</sub> </em>tersebut dikontribusi oleh transisi elektron antara pita valensi O 2<em>p</em> dan konduksi Ti 3<em>d</em><em>. </em>Susbtitusi atom La pada posisi atom Y tidak menghasilkan pita di tengah <em>E<sub>g</sub></em> (<em>intermediate band</em>) melainkan hanya memperlebar atau mempersempit celah pita pada NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> akibat distorsi panjang ikatan Ti‒O. Penelitian ini menunjukkan peran signifikan dari La terhadap sifat elektronik material NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> untuk aplikasi pada sel surya di masa depan. </p><p><strong>Modification of Electronic Properties of NaYTiO<sub>4</sub> Perovskite Material by Variation of Lanthanum Dopants Concentration using Density Functional Theory Method. </strong>Bandgap energy and density of state (DOS) of NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0; 0.25; 0.50 and 0.75) can be predicted theoretically using density functional theory (DFT) approach. The initial calculation is based on the local density approximation (LDA) and generalized gradient approximation of Perdew-Burke-Ernzerhof (GGA+PBE) as exchange-correlation functional. Initial calculations of bandgap energy and DOS were performed on conventional unit cells (1×1×1) for NaYTiO<sub>4</sub> and supercells (2×2×1) for NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0.25; 0.50 and 0.75) with the CASTEP Materials Studio program. The calculation results show the bandgap energy (<em>E<sub>g</sub></em>) of 3.447; 3.384; 3.356 and 3.560 eV for x = 0; 0.25; 0.50 and 0.75 with the LDA method. On the other hand, the GGA+PBE method shows an <em>E<sub>g</sub></em> of 3.039; 2.963 and 2.930 eV for x = 0; 0.25; 0.50 and 0.75. DOS character calculation results show that all materials exhibit the <em>E<sub>g</sub></em> transition, which is contributed by the electron transition between the O 2<em>p</em> valence band and Ti 3<em>d</em> conduction band. The substitution of La atoms at the Y atomic position does not produce a band in the middle of <em>E<sub>g</sub></em> (intermediate band) but only widens or narrows the bandgap in NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> due to distortion of the Ti‒O bond length. This study demonstrates the significant role of La on the electronic properties of NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> materials for future solar cell applications.</p>","PeriodicalId":7926,"journal":{"name":"Alchemy: Jurnal Penelitian Kimia","volume":"23 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2022-02-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Modifikasi Sifat Elektronik Material Perovskit NaYTiO4 oleh Variasi Konsentrasi Dopan Lantanum dengan Metode Density Functional Theory\",\"authors\":\"Wisanggeni Bayu Aji, H. Sutrisno\",\"doi\":\"10.20961/alchemy.18.1.53333.80-94\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Energi celah pita dan <em>density of state</em> (DOS) dari NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0; 0,25; 0,50 dan 0,75) dapat diprediksi secara teoritis menggunakan pendekatan <em>density functional theory</em> (DFT). Perhitungan awal berdasarkan atas pendekatan <em>local density approximation</em> (LDA) dan <em>generalized gradient approximation</em> dari Perdew-Burke-Ernzerhof (GGA+PBE) sebagai fungsional tukar-korelasi. Perhitungan awal energi celah pita dan DOS dilakukan pada unit sel konvensional (1×1×1) untuk NaYTiO<sub>4</sub> dan supersel (2×2×1) untuk NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0,25; 0,50 dan 0,75) dengan program CASTEP Materials Studio. Hasil perhitungan menunjukkan energi celah pita (<em>E<sub>g</sub></em>) sebesar 3,447; 3,384; 3,356 dan 3,560 eV untuk x = 0; 0,25; 0,50 dan 0,75 dengan metode LDA. Di sisi lain, metode GGA+PBE menunjukkan <em>E<sub>g</sub> </em>sebesar 3,039; 2,963 dan 2,930 eV untuk x = 0; 0,25; 0,50 dan 0,75. Hasil perhitungan karakter DOS menunjukkan bahwa seluruh material menunjukkan transisi <em>E<sub>g</sub> </em>tersebut dikontribusi oleh transisi elektron antara pita valensi O 2<em>p</em> dan konduksi Ti 3<em>d</em><em>. </em>Susbtitusi atom La pada posisi atom Y tidak menghasilkan pita di tengah <em>E<sub>g</sub></em> (<em>intermediate band</em>) melainkan hanya memperlebar atau mempersempit celah pita pada NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> akibat distorsi panjang ikatan Ti‒O. Penelitian ini menunjukkan peran signifikan dari La terhadap sifat elektronik material NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> untuk aplikasi pada sel surya di masa depan. </p><p><strong>Modification of Electronic Properties of NaYTiO<sub>4</sub> Perovskite Material by Variation of Lanthanum Dopants Concentration using Density Functional Theory Method. </strong>Bandgap energy and density of state (DOS) of NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0; 0.25; 0.50 and 0.75) can be predicted theoretically using density functional theory (DFT) approach. The initial calculation is based on the local density approximation (LDA) and generalized gradient approximation of Perdew-Burke-Ernzerhof (GGA+PBE) as exchange-correlation functional. Initial calculations of bandgap energy and DOS were performed on conventional unit cells (1×1×1) for NaYTiO<sub>4</sub> and supercells (2×2×1) for NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> (x = 0.25; 0.50 and 0.75) with the CASTEP Materials Studio program. The calculation results show the bandgap energy (<em>E<sub>g</sub></em>) of 3.447; 3.384; 3.356 and 3.560 eV for x = 0; 0.25; 0.50 and 0.75 with the LDA method. On the other hand, the GGA+PBE method shows an <em>E<sub>g</sub></em> of 3.039; 2.963 and 2.930 eV for x = 0; 0.25; 0.50 and 0.75. DOS character calculation results show that all materials exhibit the <em>E<sub>g</sub></em> transition, which is contributed by the electron transition between the O 2<em>p</em> valence band and Ti 3<em>d</em> conduction band. The substitution of La atoms at the Y atomic position does not produce a band in the middle of <em>E<sub>g</sub></em> (intermediate band) but only widens or narrows the bandgap in NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> due to distortion of the Ti‒O bond length. This study demonstrates the significant role of La on the electronic properties of NaY<sub>(1-x)</sub>La<sub>x</sub>TiO<sub>4</sub> materials for future solar cell applications.</p>\",\"PeriodicalId\":7926,\"journal\":{\"name\":\"Alchemy: Jurnal Penelitian Kimia\",\"volume\":\"23 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2022-02-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Alchemy: Jurnal Penelitian Kimia\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.20961/alchemy.18.1.53333.80-94\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Alchemy: Jurnal Penelitian Kimia","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.20961/alchemy.18.1.53333.80-94","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
裂纹能量和厚度(DOS)的NaY(1-x)LaxTiO4 (x = 0;0;可以用DFT理论来预测。初步计算是基于地方丹麦方法(LDA)和一般级梯度词典(GGA+PBE)作为功能相关的转换相关。丝带能量开始裂缝计算和DOS进行常规细胞(1×1×1)单位为NaYTiO4 supersel(2×2×1)不(1-x) LaxTiO4 (x = 0;(0.50和0.75)CASTEP材料工作室项目。计算结果显示色带间隙能量为3,447;3,384;356和3560 x = 0的eV;0;0.50和0.75与LDA的方法。另一方面,GGA+PBE的方法显示Eg等于3039;2.963和2.930 x = 0的eV;0;0。50和0。75。DOS字符计算结果表明,所有的物质都表明,移位作用是能动性O - 2p频带和Ti - 3d传导之间的电子转换。拉的原子在Y的原子位置上不会产生内膜带子,只是在内膜内(1-x)拉克斯提4的裂纹上加宽或缩小。这项研究表明,洛杉矶对未来太阳能电池应用的NaY电子材料(1-x)LaxTiO4的显著作用。通过运用二氧化二烯变量原理来修改电子特性。四弦弦的能量和密度0。25;0.50和0.75)可以预测他们使用的二分之一原理原理。最初的calculation是基于地方厌恶(LDA)和普通梯级倾向倾向于出口玉米相关的琐事。最初的calculations bandgap energy和DOS是performed on conventional单位为NaYTiO4细胞(1×1×1)和supercells(2×2×1)为不1-x) LaxTiO4 (x = 0。25;与CASTEP材料工作室项目一起进行。计算结果显示了3447的能量;3.384;x = 0的3356和3560 eV;0。25;与艾达方法共0.50和0.75。另一方面,嘎+PBE方法呈现3039;x = 0的2963和2930 eV;0。25;0。50和0。75。DOS character计算结果显示,所有的材料都显示了这种转换,这是由O 2p valence乐队和Ti 3d conduction乐队之间的电子转换结合而成的。原子的替代品在中间不能产生一支乐队,但只能在一种情况下产生乐队的缺失或狭窄。这项研究表明,洛杉矶电子属性上的巨大恶魔。
Modifikasi Sifat Elektronik Material Perovskit NaYTiO4 oleh Variasi Konsentrasi Dopan Lantanum dengan Metode Density Functional Theory
Energi celah pita dan density of state (DOS) dari NaY(1-x)LaxTiO4 (x = 0; 0,25; 0,50 dan 0,75) dapat diprediksi secara teoritis menggunakan pendekatan density functional theory (DFT). Perhitungan awal berdasarkan atas pendekatan local density approximation (LDA) dan generalized gradient approximation dari Perdew-Burke-Ernzerhof (GGA+PBE) sebagai fungsional tukar-korelasi. Perhitungan awal energi celah pita dan DOS dilakukan pada unit sel konvensional (1×1×1) untuk NaYTiO4 dan supersel (2×2×1) untuk NaY(1-x)LaxTiO4 (x = 0,25; 0,50 dan 0,75) dengan program CASTEP Materials Studio. Hasil perhitungan menunjukkan energi celah pita (Eg) sebesar 3,447; 3,384; 3,356 dan 3,560 eV untuk x = 0; 0,25; 0,50 dan 0,75 dengan metode LDA. Di sisi lain, metode GGA+PBE menunjukkan Egsebesar 3,039; 2,963 dan 2,930 eV untuk x = 0; 0,25; 0,50 dan 0,75. Hasil perhitungan karakter DOS menunjukkan bahwa seluruh material menunjukkan transisi Egtersebut dikontribusi oleh transisi elektron antara pita valensi O 2p dan konduksi Ti 3d. Susbtitusi atom La pada posisi atom Y tidak menghasilkan pita di tengah Eg (intermediate band) melainkan hanya memperlebar atau mempersempit celah pita pada NaY(1-x)LaxTiO4 akibat distorsi panjang ikatan Ti‒O. Penelitian ini menunjukkan peran signifikan dari La terhadap sifat elektronik material NaY(1-x)LaxTiO4 untuk aplikasi pada sel surya di masa depan.
Modification of Electronic Properties of NaYTiO4 Perovskite Material by Variation of Lanthanum Dopants Concentration using Density Functional Theory Method. Bandgap energy and density of state (DOS) of NaY(1-x)LaxTiO4 (x = 0; 0.25; 0.50 and 0.75) can be predicted theoretically using density functional theory (DFT) approach. The initial calculation is based on the local density approximation (LDA) and generalized gradient approximation of Perdew-Burke-Ernzerhof (GGA+PBE) as exchange-correlation functional. Initial calculations of bandgap energy and DOS were performed on conventional unit cells (1×1×1) for NaYTiO4 and supercells (2×2×1) for NaY(1-x)LaxTiO4 (x = 0.25; 0.50 and 0.75) with the CASTEP Materials Studio program. The calculation results show the bandgap energy (Eg) of 3.447; 3.384; 3.356 and 3.560 eV for x = 0; 0.25; 0.50 and 0.75 with the LDA method. On the other hand, the GGA+PBE method shows an Eg of 3.039; 2.963 and 2.930 eV for x = 0; 0.25; 0.50 and 0.75. DOS character calculation results show that all materials exhibit the Eg transition, which is contributed by the electron transition between the O 2p valence band and Ti 3d conduction band. The substitution of La atoms at the Y atomic position does not produce a band in the middle of Eg (intermediate band) but only widens or narrows the bandgap in NaY(1-x)LaxTiO4 due to distortion of the Ti‒O bond length. This study demonstrates the significant role of La on the electronic properties of NaY(1-x)LaxTiO4 materials for future solar cell applications.