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首页> 外文期刊>Journal of Materials Science >Dispersion of the linear and nonlinear optical susceptibilities of disilver germanium sulfide from DFT calculations
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Dispersion of the linear and nonlinear optical susceptibilities of disilver germanium sulfide from DFT calculations

机译:通过DFT计算得出二硫化锗的线性和非线性光学磁化率的色散

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The dispersion of the linear and nonlinear optical susceptibilities is calculated for disilver germanium sulfide (Ag_2GeS_3) using the all-electron full potential linearized augmented plane wave (FP-LAPW) method. Calculations are performed with four exchange correlations namely local density approximation (LDA), general gradient approximation (GGA), Engel-Vosko generalized gradient approximation (EVGGA), and modified Becke-Johnson potential (mBJ). Our calculations give a band gap of 0.40 eV (LDA), 0.42 eV (GGA), 1.03 eV (EVGGA), and 1.30 eV (mBJ) in comparison with our measured gap (1.98 eV). The mBJ exchange correlation gives the best agreement with experiment. We find that the calculated linear optical susceptibilities of Ag_2GeS_3 show considerable anisotropy which is useful for second harmonic generation and optical parametric oscillation. To analyze the spectra of the calculated χ _(113) ~((2)) (ω), χ _(232) ~((2)) (ω), χ _(311) ~((2)) (ω), χ _(322) ~((2)) (ω), and χ _(333) ~((2)) (ω), we have correlated the features of these spectra with the features of ε_2(ω) spectra as a function of ω/2 and ω. From the calculated dominant component |χ _(333) ~((2)) (ω)|, we find that the microscopic second-order hyperpolarizability, β_(333), the vector components along the dipole moment direction is 41.2 × 10~(-30) esu at static limit and 222.9 × 10 ~(-30) esu at λ = 1064 nm. ? 2012 Springer Science+Business Media New York.
机译:使用全电子全势线性化增强平面波(FP-LAPW)方法计算了二硫化锗(Ag_2GeS_3)的线性和非线性光学磁化率的色散。使用四个交换相关性进行计算,即局部密度近似(LDA),通用梯度近似(GGA),Engel-Vosko广义梯度近似(EVGGA)和修正的Becke-Johnson势(mBJ)。与我们测得的间隙(1.98 eV)相比,我们的计算得出的带隙为0.40 eV(LDA),0.42 eV(GGA),1.03 eV(EVGGA)和1.30 eV(mBJ)。 mBJ交换相关性与实验具有最佳一致性。我们发现,计算得出的Ag_2GeS_3的线性磁化率显示出相当大的各向异性,这对于二次谐波的产生和光学参量振荡很有用。要分析计算的χ_(113)〜((2))(ω),χ_(232)〜((2))(ω),χ_(311)〜((2))(ω ),χ_(322)〜((2))(ω)和χ_(333)〜((2))(ω),我们已将这些光谱的特征与ε_2(ω)光谱的特征相关联作为ω/ 2和ω的函数。从计算出的主导分量|χ_(333)〜((2))(ω)|中,我们发现微观二阶超极化率β_(333)沿偶极矩方向的矢量分量为41.2×10〜。静态极限下为(-30)esu,λ= 1064 nm下为222.9×10〜(-30)esu。 ? 2012年Springer Science + Business Media纽约。

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