School of Chemical and Physical Sciences, Flinders University, GPO Box 2100, Adelaide, South Australia 5001, Australia.
J Chem Phys. 2012 Aug 28;137(8):084305. doi: 10.1063/1.4746688.
Sixteen intermolecular vibrational levels of the S(0) state of the fluorobenzene-Ar van der Waals complex have been observed using dispersed fluorescence. The levels range up to ~130 cm(-1) in vibrational energy. The vibrational energies have been modelled using a complete set of harmonic and quartic anharmonic constants and a cubic anharmonic coupling between the stretch and long axis bend overtone that becomes near ubiquitous at higher energies. The constants predict the observed band positions with a root mean square deviation of 0.04 cm(-1). The set of vibrational levels predicted by the constants, which includes unobserved bands, has been compared with the predictions of ab initio calculations, which include all vibrational levels up to 70-75 cm(-1). There are small differences in energy, particularly above 60 cm(-1), however, the main differences are in the assignments and are largely due to the limitations of assigning the ab initio wavefunctions to a simple stretch, bend, or combination when the states are mixed by the cubic anharmonic coupling. The availability of these experimental data presents an opportunity to extend ab initio calculations to higher vibrational energies to provide an assessment of the accuracy of the calculated potential surface away from the minimum. The intermolecular modes of the fluorobenzene-Ar(2) trimer complex have also been investigated by dispersed fluorescence. The dominant structure is a pair of bands with a ~35 cm(-1) displacement from the origin band. Based on the set of vibrational modes calculated from the fluorobenzene-Ar frequencies, they are assigned to a Fermi resonance between the symmetric stretch and symmetric short axis bend overtone. The analysis of this resonance provides a measurement of the coupling strength between the stretch and short axis bend overtone in the dimer, an interaction that is not directly observed. The coupling matrix elements determined for the fluorobenzene-Ar stretch-long axis bend overtone and stretch-short axis bend overtone couplings are remarkably similar (3.8 cm(-1) cf. 3.2 cm(-1)). Several weak features seen in the fluorobenzene-Ar(2) spectrum have also been assigned.
十六个氟苯 - Ar 范德华复合物 S(0)态的分子间振动能级已通过分散荧光观察到。振动能级的范围高达约 130cm(-1)。使用一组完整的谐和和四次非谐常数以及拉伸和长轴弯曲泛频之间的三次非谐耦合对振动能进行了建模,这种耦合在更高的能量下变得无处不在。常数预测观察到的带位置,均方根偏差为 0.04cm(-1)。由常数预测的振动能级集,包括未观察到的带,与从头算计算的预测进行了比较,从头算计算包括高达 70-75cm(-1)的所有振动能级。能量上存在较小差异,特别是在 60cm(-1)以上,但主要差异在于分配,并且主要归因于当状态通过三次非谐耦合混合时,将从头算波函数分配给简单的拉伸、弯曲或组合的限制。这些实验数据的可用性提供了一个机会,可以将从头算计算扩展到更高的振动能,以评估远离势阱的计算势面的准确性。还通过分散荧光研究了氟苯 - Ar(2)三聚体复合物的分子间模式。主要结构是一对带,与起源带的位移约为 35cm(-1)。基于从氟苯 - Ar 频率计算的振动模式集,它们被分配给对称拉伸和对称短轴弯曲泛频之间的费米共振。该共振的分析提供了二聚体中拉伸和短轴弯曲泛频之间耦合强度的测量,这种相互作用无法直接观察到。确定的氟苯 - Ar 拉伸 - 长轴弯曲泛频和拉伸 - 短轴弯曲泛频耦合的耦合矩阵元非常相似(3.8cm(-1)cf.3.2cm(-1))。氟苯 - Ar(2)光谱中还观察到几个弱特征也已被分配。