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Alkali-metal/alkaline-earth-metal fluorine beryllium borate NaSr3Be3B3O9F4 with large nonlinear optical properties in the deep-ultraviolet region

机译:碱金属/碱土金属氟铍硼酸盐Nasr3Be3B3O9F4在深紫外区具有较大的非线性光学性质

摘要

The linear optical response and second harmonic generation (SHG) in alkali-metal/alkaline-earth-metal fluorine beryllium borate NaSr3Be3B3O9F4 are investigated by means of density functional theory. Calculations are performed using four types of exchange correlations: Ceperley-Alder local density approximation, Perdew Burke and Ernzerhof general gradient approximation, Engel-Vosko generalized gradient approximation, and the recently modified Becke-Johnson potential (mBJ). The mBJ approach brings the calculated band gap (7.20 eV) in excellent agreement with the experimental one (7.28 eV). The calculated values of the uniaxial anisotropy delta epsilon = -076 and the birefringence Delta n(0) = 052 indicate considerable anisotropy in the linear optical properties, which makes it favorable for the second harmonic generation. The dominant component of the second harmonic generation is chi((2))(111)(omega). The value of vertical bar chi((2))(111)(omega)vertical bar is about 1.2 pm/V at lambda = 1064 nm in agreement with previous calculations. To analyze the origin of the high SHG of NaSr3Be3B3O9F4 single crystals, we have correlated the features of vertical bar chi((2))(111)(omega)vertical bar spectra with the features of epsilon(2)(omega) spectra as a function of omega/2 and omega. From the calculated dominant component vertical bar chi((2))(111)(omega)vertical bar, we find that the microscopic first hyperpolarizability, beta(111), the vector components along the dipole moment direction is 0.5 x 10(-30) esu at static limit and 0.6 x 10(-30) esu at lambda = 1064 nm. ud
机译:利用密度泛函理论研究了碱金属/碱土金属氟硼酸铍钠NaSr3Be3B3O9F4中的线性光学响应和二次谐波(SHG)的产生。计算使用四种类型的交换相关性进行:Ceperley-Alder局部密度近似,Perdew Burke和Ernzerhof广义梯度近似,Engel-Vosko广义梯度近似以及最近修改的Becke-Johnson势(mBJ)。 mBJ方法使计算出的带隙(7.20 eV)与实验值(7.28 eV)非常吻合。单轴各向异性Δε= -076和双折射Δn(0)= 052的计算值表明线性光学性质中的各向异性较大,这使其有利于二次谐波的产生。二次谐波产生的主要成分是chi((2))(111)Ω。与先前的计算结果一致,在λ= 1064 nm时,垂直条chi((2))(111)Ω垂直条的值约为1.2 pm / V。为了分析NaSr3Be3B3O9F4单晶的高SHG的起源,我们将垂直条形chi((2))(111)(omega)垂直条形图的特征与epsilon(2)(omega)谱图的特征相关联omega / 2和omega的功能。从计算出的主导分量垂直条chi((2))(111)Ω垂直条中,我们发现微观第一超极化率beta(111)沿偶极矩方向的矢量分量为0.5 x 10(-30) )在静态极限处的esu和在lambda = 1064 nm处的0.6 x 10(-30)esu。 ud

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