Department of Chemistry, University of Basel, Basel, Switzerland.
J Phys Chem A. 2011 May 26;115(20):5053-61. doi: 10.1021/jp202503m. Epub 2011 May 4.
The vibrationally excited cyanide ion (CN(-)) in H2O or D2O relaxes back to the ground state within several tens of picoseconds. Pump-probe infrared spectroscopy has determined relaxation times of T1 = 28 ± 7 and 71 ± 3 ps in H2O and D2O, respectively. Atomistic simulations of this process using nonequilibrium molecular dynamics simulations allow determination of whether it is possible at all to describe such a process, what level of accuracy in the force fields is required, and whether the information can be used to understand the molecular mechanisms underlying vibrational relaxation. It is found that, by using the best electrostatic models investigated, absolute relaxation times can be described rather more qualitatively (T1(H2O) = 19 ps and T1(D2O) = 34 ps) whereas the relative change in going from water to deuterated water is more quantitatively captured (factor of 2 vs 2.5 from experiment). However, moderate adjustment of the van der Waals ranges by less than 20% (for NVT) and 7.5% (for NVE), respectively, leads to almost quantitative agreement with experiment. Analysis of the energy redistribution establishes that the major pathway for CN(-) relaxation in H2O or D2O proceeds through coupling to the water-bending plus libration mode.
在 H2O 或 D2O 中,振动激发的氰化物离子 (CN(-)) 在几十皮秒内回到基态。泵浦探测红外光谱法确定了在 H2O 和 D2O 中分别为 T1 = 28 ± 7 和 71 ± 3 ps 的弛豫时间。使用非平衡分子动力学模拟对该过程的原子模拟允许确定是否有可能描述这样的过程,力场需要达到何种精度水平,以及信息是否可用于理解振动弛豫的分子机制。结果发现,通过使用研究中最好的静电模型,可以更定性地描述绝对弛豫时间(T1(H2O) = 19 ps 和 T1(D2O) = 34 ps),而从水到氘化水的相对变化则更定量地捕获(实验中为 2 倍与 2.5 倍)。然而,通过将范德华范围适度调整小于 20%(对于 NVT)和 7.5%(对于 NVE),分别与实验几乎完全吻合。能量再分配的分析表明,CN(-)在 H2O 或 D2O 中的弛豫的主要途径是通过与水弯曲加简谐振动模式耦合。