Department of Physical Chemistry II, Ruhr-University Bochum, Germany.
Phys Chem Chem Phys. 2015 May 7;17(17):11898-907. doi: 10.1039/c5cp01035g.
In continuation of earlier work on La(III), Ni(II) and Mn(II) halides, we present low frequency (30-400 cm(-1)) spectra of solvated HCl and HBr as a function of solute concentration. This frequency range provides direct access to water network modes and changes induced by solvated solutes. We were able to dissect the spectra into components associated to solvated ions and ion pairs using a chemical equilibrium model in combination with principal component analysis. While the Cl(-) rattling mode at 190 cm(-1) is found to be unchanged, the Br(-) resonance around 90 cm(-1) is decreased in intensity below the detection threshold when replacing the divalent or trivalent metal ions by a proton. The solvated proton shows two resonances: a solvation water mode around 140 cm(-1) and a high frequency resonance at 325 cm(-1) that we assign to the rattling motion of an Eigen structure H3O(+) in its solvation cage. This assignment is corroborated by isotopic substitution measurements which show a redshift of the high frequency peak when HCl/H2O is replaced by DCl/D2O. The linewidth of the H3O(+) rattling mode corresponds to a relaxation time of the oscillatory process of τ ≈ 60 fs, considerably faster than the relaxation time of τ ≈ 160 fs for Cl(-). In addition, we find a broad background that we attribute to fast non-oscillatory motions of a proton in a Zundel-like complex. Our results are in agreement with an Eigen-Zundel-Eigen (EZE) model of proton transport. Upon ion pairing the broad background is strongly reduced indicating a reduction of fast proton transfer processes. The Cl(-) resonance blueshifts by 20 cm(-1) which indicates a transition from free ions to a solvent shared ion pair. Surprisingly, the center frequency of the Eigen complex does not change upon ion pairing. This can be rationalized in terms of an unchanged local solvation structure.
延续早期关于 La(III)、Ni(II) 和 Mn(II)卤化物的工作,我们呈现了溶剂化 HCl 和 HBr 的低频(30-400 cm(-1))谱作为溶质浓度的函数。这个频率范围直接提供了对水网络模式和溶剂化溶质引起的变化的访问。我们能够使用化学平衡模型结合主成分分析将光谱分解为与溶剂化离子和离子对相关的分量。虽然在 190 cm(-1)处发现 Cl(-)的振动态不变,但当二价或三价金属离子被质子取代时,90 cm(-1)左右的 Br(-)共振的强度降低到检测阈值以下。溶剂化质子显示出两个共振:一个围绕 140 cm(-1)的溶剂化水分子模式和一个在 325 cm(-1)处的高频共振,我们将其归因于其溶剂笼中的 Eigen 结构 H3O(+)的振动态。这种分配得到了同位素取代测量的证实,当 HCl/H2O 被 DCl/D2O 取代时,高频峰发生红移。H3O(+)振动态的线宽对应于振荡过程的弛豫时间 τ≈60 fs,比 Cl(-)的弛豫时间 τ≈160 fs快得多。此外,我们发现一个宽的背景,我们将其归因于质子在 Zundel 类似物中的快速非振荡运动。我们的结果与质子传输的 Eigen-Zundel-Eigen (EZE) 模型一致。在离子对形成后,宽背景大大减少,表明快速质子转移过程减少。Cl(-)共振蓝移 20 cm(-1),表明从自由离子到共享溶剂的离子对的转变。令人惊讶的是,Eigen 复合物的中心频率在离子对形成后没有变化。这可以根据不变的局部溶剂化结构来合理化。