Yuan Rongfeng, Yan Chang, Tamimi Amr, Fayer Michael D
Department of Chemistry, Stanford University , Stanford, California 94305, United States.
J Phys Chem B. 2015 Oct 22;119(42):13407-15. doi: 10.1021/acs.jpcb.5b08168. Epub 2015 Oct 12.
The dynamic nature of hydrogen bonding between a molecular anion, selenocyanate (SeCN(-)), and water in aqueous solution (D2O) is addressed using FT-IR spectroscopy, two-dimensional infrared (2D IR) vibrational echo spectroscopy, and polarization selective IR pump-probe (PSPP) experiments performed on the CN stretching mode. The CN absorption spectrum is asymmetric with a wing on the low frequency (red) side of the line in contrast to the spectrum in the absence of hydrogen bonding. It is shown that the red wing is the result of an increase in the CN stretch transition dipole moment due to the effect of hydrogen bonding (non-Condon effect). This non-Condon effect is similar in nature to observations on pure water and other nonionic systems where hydrogen bonding enhances the extinction coefficient. The 2D IR measurements of spectral diffusion (solvent structural evolution) yield a time constant of 1.5 ps, which is within error the same as that of the OH stretch of HOD in D2O (1.4 ps). The orientational relaxation of SeCN(-) measured by PSPP experiments is long (4.04 ps) compared to the spectral diffusion time. The population decay at or near the absorption line center is a single-exponential decay of 37.4 ± 0.3 ps, the vibrational lifetime. However, on the red side of the line the decay is biexponential with a low amplitude, fast component; on the blue side of the line there is a low amplitude, fast growth followed by the lifetime decay. Both of the fast components have 1.5 ps time constants, which is the spectral diffusion time. The fast components of the population decays are the results of the non-Condon effect that causes the red side of the line to be over pumped by the pump pulse. Spectral diffusion then produces the fast decay component on the red side of the line and the growth on the blue side of the line as the excess initial population on the red side produces a net population flow from red to blue.
利用傅里叶变换红外光谱(FT-IR)、二维红外(2D IR)振动回波光谱以及对氰基(CN)伸缩模式进行的偏振选择性红外泵浦-探测(PSPP)实验,研究了分子阴离子硒氰酸根(SeCN(-))与重水溶液(D2O)中的水之间氢键的动态性质。与不存在氢键时的光谱相比,CN吸收光谱不对称,在谱线的低频(红色)一侧有一个拖尾。结果表明,红色拖尾是由于氢键作用(非康登效应)导致CN伸缩跃迁偶极矩增加的结果。这种非康登效应在本质上与对纯水和其他非离子体系的观察结果相似,在这些体系中氢键增强了消光系数。光谱扩散(溶剂结构演化)的二维红外测量得到的时间常数为1.5皮秒,与D2O中HOD的OH伸缩时间常数(1.4皮秒)在误差范围内相同。通过PSPP实验测量的SeCN(-)的取向弛豫时间较长(4.04皮秒),与光谱扩散时间相比。吸收线中心或其附近的布居衰减是37.4±0.3皮秒的单指数衰减,即振动寿命。然而,在谱线的红色一侧,衰减是双指数的,有一个低幅度、快速的分量;在谱线的蓝色一侧,有一个低幅度、快速的增长,随后是寿命衰减。两个快速分量的时间常数均为1.5皮秒,即光谱扩散时间。布居衰减的快速分量是由非康登效应导致的,该效应使谱线的红色一侧被泵浦脉冲过度泵浦。然后,光谱扩散在谱线的红色一侧产生快速衰减分量,在谱线的蓝色一侧产生增长,因为红色一侧过量的初始布居产生了从红色到蓝色的净布居流。