Chemistry Department, Wrocław University of Technology, Wyb. St. Wyspiańskiego 27, 50-370 Wrocław, Poland.
J Comput Chem. 2011 Mar;32(4):718-29. doi: 10.1002/jcc.21665. Epub 2010 Oct 5.
Potential energy surface (PES) of thiourea, SC(NH(2))(2), has been searched for stable conformers under C(1), C(s), C(2), and C(2v) symmetry constraints by post-Hartree-Fock ab initio methods with electron correlation level varying from second-order Moeller-Plesset perturbation theory (MP2) to quadratic configuration interaction with single and double excitations (QCISD) and basis sets of double- and triple-zeta quality within 6-31+G(d,p) to aug-cc-pVTZ range. Thiourea conformers of C(2) and C(s) symmetry have been found as stationary points on the PES with no imaginary frequencies at MP2/6-31+G(d,p) level, whereas only the C(2) conformer seems as true minimum when basis sets containing more polarization and/or diffuse functions were used. At QCISD/cc-pVTZ level, only the C(2) thiourea conformer has been found as true minimum on the PES. Anharmonic vibrational spectra of C(2) conformers of thiourea and thiourea-d(4) have been computed by vibrational self-consistent field (VSCF) and correlation-corrected VSCF methods using quartic force field approximation at MP2/TZV+(2d,2p), and MP2/6-311+G(3df,2p) level and direct approach at MP2/6-31+G(2d,p) level. Both quartic force field and direct VSCF methods used PES expansion in curvilinear (internal) coordinates. Wavenumbers of fundamental, first overtone, and combination transitions of C(2) symmetry conformer have been calculated for natural abundance thiourea and thiourea-d(4) isotopomer. Anharmonic corrections originating from mean field and mode coupling effects vary from 5 to 60 cm(-1), whereas mode-mode correlation contribution seems significant in the case of ν(N-H) stretching and δ(NH(2)) deformation modes (15-5 cm(-1)). Application of internal coordinates in the VSCF calculation results in slight underestimation of δ(NH(2)) deformation mode fundamentals and correct description of out-of-plane large-amplitude τ(SCNH) modes.
硫脲(SC(NH(2))(2))的势能面(PES)在 C(1)、C(s)、C(2)和 C(2v) 对称约束下,通过二阶 Moeller-Plesset 微扰理论 (MP2) 到二次组态相互作用(QCISD)与双和三重 zeta 质量的基组进行了从头算搜索,范围从 6-31+G(d,p)到 aug-cc-pVTZ。在 MP2/6-31+G(d,p)水平下,在 C(2)和 C(s)对称的硫脲构象作为 PES 上的稳定点,没有虚频,而只有当使用包含更多极化和/或弥散函数的基组时,C(2)构象才被认为是真正的最小值。在 QCISD/cc-pVTZ 水平下,只有 C(2)硫脲构象被认为是 PES 上的真正最小值。使用四极力场近似,在 MP2/TZV+(2d,2p)和 MP2/6-311+G(3df,2p)水平以及 MP2/6-31+G(2d,p)水平下,通过振动自洽场(VSCF)和相关校正的 VSCF 方法,计算了 C(2)构象的硫脲和硫脲-d(4)的非谐振动光谱。两种四极力场和直接 VSCF 方法都使用了曲线(内部)坐标的 PES 展开。计算了天然丰度硫脲和硫脲-d(4)同位异构体的 C(2)对称构象的基本、第一泛音和组合跃迁的波数。源于平均场和模式耦合效应的非谐校正从 5 到 60 cm(-1),而ν(N-H)伸缩和δ(NH(2))变形模式的模式-模式相关贡献似乎很显著(15-5 cm(-1))。在 VSCF 计算中应用内部坐标会导致δ(NH(2))变形模式基本的轻微低估,并正确描述了面外大振幅τ(SCNH)模式。