采用基于第一性原理下的局域密度近似(LDA)方法对岩石矿物结构Ca硫族化合物CaX(X=S, Se, Te)的晶格常数和电子结构进行了研究.研究结果表明,使用LDA方法得到的晶格常数与实验值符合得很好,但带隙值却远低于实验值.为了获得可靠的带隙值...采用基于第一性原理下的局域密度近似(LDA)方法对岩石矿物结构Ca硫族化合物CaX(X=S, Se, Te)的晶格常数和电子结构进行了研究.研究结果表明,使用LDA方法得到的晶格常数与实验值符合得很好,但带隙值却远低于实验值.为了获得可靠的带隙值,使用了GW(G格林函数, W库伦屏蔽相互作用)近似方法对Ca硫族化合物的带隙进行修正.利用GW近似方法计算CaS和CaSe的带隙值比利用LDA计算的带隙值高,并且与实验值相吻合.同时也预测了CaTe的带隙值,尽管没有实验值作为参考,但GW近似计算的结果应该是合适的值.展开更多
Structural, electronic, and optical properties of alloys BexMgl-xX （X = S, Se, Te） in the assortment 0 〈 x 〈 1 were theoretically reported for the first time in zinc-blende （ZB） phase. The calculations were carr...Structural, electronic, and optical properties of alloys BexMgl-xX （X = S, Se, Te） in the assortment 0 〈 x 〈 1 were theoretically reported for the first time in zinc-blende （ZB） phase. The calculations were carried out by using full-potential linearized augmented plane wave plus local orbitals （FP-LAPW＋lo） formalism contained by the framework of density functional theory （DFT）. Wu--Cohen （WC） generalized gradient approximation （GGA）, based on optimization energy, has been applied to calculate these theoretical results. In addition, we used Becke and Johnson （mBJ-GGA） potential, modified form of GGA functional, to calculate electronic structural properties up to a high precision degree. The alloys were composed with the concentrations x = 0.25, 0.5, and 0.75 in pursuance of ＇special quasi-random structures＇ （SQS） approach of Zunger for the restoration of disorder around the observed site of alloys in the first few shells. The structural parameters have been predicted by minimizing the total energy in correspondence of unit cell volume. Our alloys established direct band gap at different concentrations that make their importance in optically active materials. Furthermore, density of states was discussed in terms of the contribution of Be and Mg s and chalcogen （S, Se, and Te） s and p states and observed charge density helped us to investigate the bonding nature. By taking into consideration of immense importance in optoelectronics of these materials, the complex dielectric function was calculated for incident photon energy in the range 0--15 eV.展开更多
Using experimental values of the structure factor of liquid Se1-xTex(x =0. 0, 0. 6, 0. 7, 0. 8, 1. 0. ) alloys measured by Takeda et al., the potential functions at different compositions are derived from Rao-Joarder&...Using experimental values of the structure factor of liquid Se1-xTex(x =0. 0, 0. 6, 0. 7, 0. 8, 1. 0. ) alloys measured by Takeda et al., the potential functions at different compositions are derived from Rao-Joarder'S equation. From the change of the shape of the potential function at different compositions, we can infer that when x is between 0. 7 and 0. 8 the nonmetal-metal transition occurs in this system. This is the first time to use the calculation of the potential function to find the NM-M transition Furthermore we give the longitudinal and transverse phonon frequencies by using Bhatia-Singh'S model. Then the elastic constants are computed. Using the potential function, the characteristic frequency is obtained and compared with the average frequency, Debye frequency, and the maximum longitudinal frequency compute4 by other methods. Finally, we compare the sound velocities calculated from the elastic constants in the long-wave limit with corresponding experimental values.展开更多
文摘采用基于第一性原理下的局域密度近似(LDA)方法对岩石矿物结构Ca硫族化合物CaX(X=S, Se, Te)的晶格常数和电子结构进行了研究.研究结果表明,使用LDA方法得到的晶格常数与实验值符合得很好,但带隙值却远低于实验值.为了获得可靠的带隙值,使用了GW(G格林函数, W库伦屏蔽相互作用)近似方法对Ca硫族化合物的带隙进行修正.利用GW近似方法计算CaS和CaSe的带隙值比利用LDA计算的带隙值高,并且与实验值相吻合.同时也预测了CaTe的带隙值,尽管没有实验值作为参考,但GW近似计算的结果应该是合适的值.
基金the Deanship of Scientific Research at King Saud University for funding this Research group No.RG 1435-004
文摘Structural, electronic, and optical properties of alloys BexMgl-xX （X = S, Se, Te） in the assortment 0 〈 x 〈 1 were theoretically reported for the first time in zinc-blende （ZB） phase. The calculations were carried out by using full-potential linearized augmented plane wave plus local orbitals （FP-LAPW＋lo） formalism contained by the framework of density functional theory （DFT）. Wu--Cohen （WC） generalized gradient approximation （GGA）, based on optimization energy, has been applied to calculate these theoretical results. In addition, we used Becke and Johnson （mBJ-GGA） potential, modified form of GGA functional, to calculate electronic structural properties up to a high precision degree. The alloys were composed with the concentrations x = 0.25, 0.5, and 0.75 in pursuance of ＇special quasi-random structures＇ （SQS） approach of Zunger for the restoration of disorder around the observed site of alloys in the first few shells. The structural parameters have been predicted by minimizing the total energy in correspondence of unit cell volume. Our alloys established direct band gap at different concentrations that make their importance in optically active materials. Furthermore, density of states was discussed in terms of the contribution of Be and Mg s and chalcogen （S, Se, and Te） s and p states and observed charge density helped us to investigate the bonding nature. By taking into consideration of immense importance in optoelectronics of these materials, the complex dielectric function was calculated for incident photon energy in the range 0--15 eV.
文摘Using experimental values of the structure factor of liquid Se1-xTex(x =0. 0, 0. 6, 0. 7, 0. 8, 1. 0. ) alloys measured by Takeda et al., the potential functions at different compositions are derived from Rao-Joarder'S equation. From the change of the shape of the potential function at different compositions, we can infer that when x is between 0. 7 and 0. 8 the nonmetal-metal transition occurs in this system. This is the first time to use the calculation of the potential function to find the NM-M transition Furthermore we give the longitudinal and transverse phonon frequencies by using Bhatia-Singh'S model. Then the elastic constants are computed. Using the potential function, the characteristic frequency is obtained and compared with the average frequency, Debye frequency, and the maximum longitudinal frequency compute4 by other methods. Finally, we compare the sound velocities calculated from the elastic constants in the long-wave limit with corresponding experimental values.
