首页> 外文期刊>The Journal of Chemical Physics >The calculation of the static first and second susceptibilities of crystalline urea: A comparison of Hartree–Fock and density functional theory results obtained with the periodic coupled perturbed Hartree–Fock/Kohn–Sham scheme
【24h】

The calculation of the static first and second susceptibilities of crystalline urea: A comparison of Hartree–Fock and density functional theory results obtained with the periodic coupled perturbed Hartree–Fock/Kohn–Sham scheme

机译:结晶尿素的静态第一和第二磁化率的计算:Hartree-Fock和密度泛函理论结果与周期耦合扰动Hartree-Fock / Kohn-Sham方案的比较

获取原文
获取原文并翻译 | 示例
           

摘要

The static polarizability α and first hyperpolarizability β tensors of crystalline urea and the corresponding first-(χ~((1))) and second-(χ~((2))) susceptibilities are calculated and compared to the same quantities obtained for the molecule by using the same code (a development version of CRYSTAL), basis set, and level of theory. In order to separate geometrical and solid state effects, two geometries are considered for the molecule in its planar conformation: (i) as cut out from the bulk structure and (ii) fully optimized. First, the effect of basis sets on computed properties is explored at the B3LYP level by employing basis sets of increasing complexity, from 6-31G(d,p) to 6-311G(2df,2pd) (Pople’s family) and from DZP to QZVPPP (Thakkar/Ahlrichs/Dunning’s family) on α and β for both the molecule and the bulk. Then, five different levels of theory, namely, SVWN (local density approximation), PBE (generalized gradient approximation), PBE0 and B3LYP (hybrid), and Hartree–Fock are compared in combination with a TZPP basis set. Present results show that hybrid methods, in particular, B3LYP, are remarkably successful in predicting correctly both the first and second susceptibilities of urea bulk when combined at least with a triple-zeta quality basis set containing a double set of polarization functions. It is also shown that diffuse functions that are needed for molecular calculations are less crucial for the crystalline structure, as expected. Indeed, B3LYP/TZPP computed χ~((1)) and χ~((2)) tensor components (χ_(aa)~((1))=1.107, χ_(cc)~((1))=1.459, and χ~((2))=-0.93 a.u.) are in very good agreement with experimental values. At variance with respect to previous periodic ab initio calculations, but in agreement with recent supermolecular results, the negative sign of χ~((2)) is confirmed. Overall, static linear and nonlinear optical properties such as dielectric constants, refractive, and birefringence indices and second-harmonic generation coefficient of crystalline urea are very well reproduced by present calculations.
机译:计算结晶尿素的静态极化率α和第一超极化率β张量以及相应的第一(χ〜((1)))和第二(χ〜((2)))磁化率,并将其与获得的相同量进行比较分子使用相同的代码(CRYSTAL的开发版本),基础集和理论水平。为了分离几何效应和固态效应,考虑分子在其平面构象中的两个几何形状:(i)从主体结构切出的和(ii)完全优化的。首先,通过使用从6-31G(d,p)到6-311G(2df,2pd)(Pople族)和从DZP到QZVPPP(Thakkar / Ahlrichs / Dunning家族)在分子和主体上都位于α和β上。然后,结合TZPP基集,比较了五个不同的理论水平,即SVWN(局部密度近似),PBE(广义梯度近似),PBE0和B3LYP(混合)以及Hartree-Fock。目前的结果表明,混合方法,特别是B3LYP,在至少与包含双重极化函数的三重质素基组结合使用时,在正确预测尿素体积的第一和第二磁化率方面非常成功。还表明,如预期的那样,分子计算所需的扩散函数对晶体结构的重要性不高。实际上,B3LYP / TZPP计算出χ〜((1))和χ〜((2))张量分量(χ_(aa)〜((1))= 1.107,χ_(cc)〜((1))= 1.459,且χ〜((2))=-0.93 au)与实验值非常吻合。相对于以前的周期性从头计算,但与最近的超分子结果一致,证实了χ〜((2))的负号。总体而言,目前的计算可以很好地再现静态线性和非线性光学性质,例如结晶尿素的介电常数,折射率和双折射指数以及二次谐波产生系数。

著录项

相似文献

  • 外文文献
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号