Mosely Jacquelyn J, Tschumper Gregory S
Department of Chemistry and Biochemistry, University of Mississippi, University, Mississippi 38677-1848, United States.
J Phys Chem A. 2024 Jul 18;128(28):5637-5645. doi: 10.1021/acs.jpca.4c03430. Epub 2024 Jul 8.
This study systematically examines the interactions of the trigonal bipyramidal silicon pentafluoride and octahedral silicon hexafluoride anions with either one or two water molecules, (SiF(HO) and SiF(HO), respectively, where = 1, 2). Full geometry optimizations and subsequent harmonic vibrational frequency computations are performed using the CCSD(T) method with a triple-ζ correlation consistent basis set augmented with diffuse functions on all non-hydrogen atoms (cc-pVTZ for H and aug-cc-pVTZ for Si, O, and F; denoted as haTZ). Two monohydrate and six dihydrate minima have been identified for the SiF(HO) systems, whereas one monohydrate and five dihydrate minima have been identified for the SiF(HO) systems. Both monohydrated anions have a minimum in which the water molecule adopts a symmetric double ionic hydrogen bond (DIHB) motif with symmetry. However, a second unique monohydrate minimum has been identified for SiF in which the water molecule adopts an asymmetric DIHB motif along the edge of the trigonal bipyramidal anion between one axial and one equatorial F atom. This structure is more than 2 kcal mol lower in energy than the local minimum at the CCSD(T)/haTZ level of theory. While the interactions between the solvent and ionic solute are quite strong for the monohydrated anions (electronic dissociation energies of ≈12 and ≈24 kcal mol for the SiF(HO) and SiF(HO) global minima, respectively), these values are nearly perfectly doubled for the dihydrates, with the lowest-energy SiF(HO) and SiF(HO) minima exhibiting dissociation energies of ≈24 and ≈47 kcal mol, respectively. Structures that form hydrogen bonds between the solvating water molecules also exhibit the largest shifts in the harmonic OH stretching frequencies for the waters of hydration. These shifts can exceed -100 cm for the SiF(HO) minimum and -300 cm for the SiF(HO) minimum relative to an isolated HO molecule at the CCSD(T)/haTZ level of theory. This work also corrects the OH stretching frequency shifts for two dihydrate minima of PF that were previously erroneously reported ( 2020, 124, 8744-8752, DOI: 10.1021/acs.jpca.0c06466).
本研究系统地考察了三角双锥构型的五氟化硅阴离子和八面体构型的六氟化硅阴离子与一个或两个水分子(分别为SiF(HO) 和SiF(HO),其中 = 1, 2)之间的相互作用。使用CCSD(T)方法并采用三ζ相关一致基组,对所有非氢原子添加弥散函数(氢原子用cc-pVTZ,硅、氧和氟原子用aug-cc-pVTZ;记为haTZ)进行了全几何优化及随后的简谐振动频率计算。对于SiF(HO)体系,已确定了两个一水合物和六个二水合物极小值,而对于SiF(HO)体系,已确定了一个一水合物和五个二水合物极小值。两种一水合阴离子均有一个极小值,其中水分子采取具有 对称性的对称双离子氢键(DIHB) motif。然而,对于SiF已确定了第二个独特的一水合物极小值,其中水分子沿着三角双锥阴离子的一条边,在一个轴向氟原子与一个赤道氟原子之间采取不对称DIHB motif。在CCSD(T)/haTZ理论水平下,这种结构的能量比 局部极小值低2 kcal mol以上。虽然对于一水合阴离子,溶剂与离子溶质之间的相互作用相当强(SiF(HO)和SiF(HO)全局极小值的电子离解能分别约为12和24 kcal mol),但对于二水合物,这些值几乎完美地翻倍,能量最低的SiF(HO)和SiF(HO)极小值的离解能分别约为24和47 kcal mol。在溶剂化水分子之间形成氢键的结构在水合水分子的简谐OH伸缩频率上也表现出最大的位移。在CCSD(T)/haTZ理论水平下,相对于孤立的HO分子,对于SiF(HO)极小值,这些位移可超过-100 cm,对于SiF(HO)极小值可超过-300 cm。这项工作还纠正了之前错误报道的PF两种二水合物极小值的OH伸缩频率位移( 2020, 124, 8744 - 8752, DOI: 10.1021/acs.jpca.0c06466)。