Antony Jens, von Helden Gert, Meijer Gerard, Schmidt Burkhard
Freie Universität Berlin, Institute of Mathematics II, Arnimalle 2-6, D-14195 Berlin, Germany.
J Chem Phys. 2005 Jul 1;123(1):014305. doi: 10.1063/1.1947191.
Anharmonic vibrational calculations for the benzoic acid monomer and dimer in the mid-IR regime (500-1800 cm(-1)) are reported. Harmonic frequencies and intensities are obtained at the DFT/B3LYP level of theory employing D95(d,p) and cc-pVTZ basis sets. Anharmonic corrections obtained from standard perturbation theory lead to redshifts of 1%-3%. In almost all cases, the resulting frequencies deviate by less than 1% from previous measurements [Bakker et al., J. Chem. Phys. 119, 11180 (2003)]. Calculated intensities are in qualitative agreement with the absorption experiment, with the cc-pVTZ values being superior to the D95(d,p) ones for a few modes of the dimer. The antisymmetric out-of-plane bending mode of the dimer, which is strongly blueshifted with respect to the monomer frequency, represents a remarkable exception: The harmonic frequencies obtained for the two basis sets differ notably from each other, and the anharmonically corrected frequencies deviate from the experimental value by 8% [D95(d,p)] or 3% (cc-pVTZ). Nonperturbative calculations in reduced dimensionality reveal that the relatively small total anharmonic shift (few tens of cm(-1)) comprises of partly much larger contributions (few hundreds of cm(-1)) which are mostly canceling each other. Many of the individual anharmonic couplings are beyond the validity of second-order perturbation theory based on cubic and semidiagonal quartic force constants only. This emphasizes the need for high-dimensional, nonperturbative anharmonic calculations at high quantum-chemical level when accurate frequencies of H-atom vibrations in double hydrogen bonds are sought for.
报道了苯甲酸单体和二聚体在中红外区域(500 - 1800 cm⁻¹)的非谐振动计算。在采用D95(d,p)和cc-pVTZ基组的密度泛函理论(DFT)/B3LYP水平上获得了谐频和谐振强度。从标准微扰理论得到的非谐校正导致了1% - 3%的红移。在几乎所有情况下,所得频率与先前的测量值[Bakker等人,《化学物理杂志》119, 11180 (2003)]的偏差小于1%。计算得到的强度与吸收实验在定性上一致,对于二聚体的一些模式,cc-pVTZ值优于D95(d,p)值。二聚体的反对称面外弯曲模式相对于单体频率有强烈的蓝移,这是一个显著的例外:两个基组得到的谐频彼此显著不同,并且非谐校正后的频率与实验值的偏差为8% [D95(d,p)]或3%(cc-pVTZ)。降维的非微扰计算表明,相对较小的总非谐位移(几十cm⁻¹)部分由大得多的贡献(几百cm⁻¹)组成,这些贡献大多相互抵消。许多单独的非谐耦合超出了仅基于立方和半对角四次力常数的二阶微扰理论的有效性范围。这强调了在寻求双氢键中H原子振动的精确频率时,需要在高量子化学水平上进行高维非微扰非谐计算。