Dipartimento di Chimica IFM, Università di Torino and NIS-Nanostructured Interfaces and Surfaces, Centre of Excellence, Via P. Giuria 7, 10125 Torino, Italy.
J Chem Phys. 2009 Dec 7;131(21):214704. doi: 10.1063/1.3267861.
The static polarizability alpha and first hyperpolarizability beta tensors of crystalline urea and the corresponding first-(chi((1))) and second-(chi((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 alpha and beta 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 chi((1)) and chi((2)) tensor components (chi(aa) ((1))=1.107, chi(cc) ((1))=1.459, and chi((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 chi((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.
我们计算了晶体尿素的静态极化率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,并将其与使用相同代码(CRYSTAL 的开发版本)、基组和理论水平获得的分子的相同量进行了比较。为了分离几何和固态效应,我们考虑了分子在其平面构象中的两种几何形状:(i)从块状结构中切出,(ii)完全优化。首先,通过使用从 6-31G(d,p)到 6-311G(2df,2pd)(Pople 家族)和从 DZP 到 QZVPPP(Thakkar/Ahlrichs/Dunning 家族)的越来越复杂的基组,在 B3LYP 水平上探索了基组对计算性质的影响,对于分子和块状物的α和β。然后,比较了五种不同的理论水平,即 SVWN(局域密度近似)、PBE(广义梯度近似)、PBE0 和 B3LYP(杂化)和 Hartree-Fock,结合 TZPP 基组。目前的结果表明,杂化方法,特别是 B3LYP,在与至少包含一组双极化函数的三重 zeta 质量基组结合时,非常成功地正确预测了尿素块状物的第一和第二磁化率。还表明,对于晶体结构,分子计算所需的弥散函数并不那么关键,这是意料之中的。实际上,B3LYP/TZPP 计算的 χ((1))和 χ((2))张量分量(χ(aa) ((1))=1.107、 χ(cc) ((1))=1.459 和 χ((2))=-0.93 a.u.)与实验值非常吻合。与以前的周期性从头算计算不同,但与最近的超分子结果一致, χ((2))的负号得到了确认。总体而言,晶体尿素的静态线性和非线性光学性质,如介电常数、折射率和双折射指数以及二次谐波产生系数,都很好地通过本计算得到了重现。