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Co⁺(CH₄)n 和 Ni⁺(CH₄)n(n = 1 - 4)的振动光谱

Vibrational spectroscopy of Co⁺(CH₄)n and Ni⁺(CH₄)n (n = 1-4).

作者信息

Kocak Abdulkadir, Sallese Zachary, Johnston Michael D, Metz Ricardo B

机构信息

Department of Chemistry, University of Massachusetts Amherst , Amherst, Massachusetts 01003, United States.

出版信息

J Phys Chem A. 2014 May 8;118(18):3253-65. doi: 10.1021/jp500617n. Epub 2014 Apr 28.

DOI:10.1021/jp500617n
PMID:24739017
Abstract

Vibrational spectra of M(+)(CH4)m(Ar)(3-m) and M(+)(CH4)n (M = Co, Ni; m = 1, 2; n = 3, 4) in the C-H stretching region (2500-3100 cm(-1)) are measured using photofragment spectroscopy, monitoring the loss of argon or methane. Interaction with the metal leads to large red shifts in the C-H stretches for proximate hydrogens. The extent of this shift is sensitive to the coordination (η(2) vs η(3)) and to the metal-methane distance. The structures of the complexes are determined by comparing measured spectra with those calculated for candidate structures at the B3LYP/6-311++G(3df,3pd) level. Binding energies are also computed using the CAM-B3LYP functional. In all cases, CH4 shows η(2) coordination to the metal. The m = 1 complexes show very large red shifts of 370 cm(-1) (for M = Co) and 320 cm(-1) (for M = Ni) in the lowest C-H stretch, relative to the symmetric stretch of free CH4. They adopt a C2v structure with the heavy atoms and proximate hydrogen atoms coplanar. The m = 2 complexes have slightly reduced red shifts, and Tee-shaped structures. Both Tee-shaped and equilateral (or quasi-equilateral) structures are observed for the n = 3 complexes. The measured photodissociation onset and significantly reduced intensity for low-frequency C-H stretches imply a value of 2650 ± 50 cm(-1) for the binding energy of Ni(+)(CH4)2-CH4. The Co(+)(CH4)4 complexes have two low-lying structures, quasi-tetrahedral and distorted square-planar, which contribute to the rich spectrum. In contrast, the symmetrical, square-planar Ni(+)(CH4)4 complex is characterized by a very simple vibrational spectrum.

摘要

利用光解离光谱法,通过监测氩气或甲烷的损失,测量了M(+)(CH4)m(Ar)(3 - m)和M(+)(CH4)n(M = Co、Ni;m = 1、2;n = 3、4)在C - H伸缩振动区域(2500 - 3100 cm(-1))的振动光谱。与金属的相互作用导致相邻氢原子的C - H伸缩振动出现大幅红移。这种红移的程度对配位方式(η(2)与η(3))以及金属 - 甲烷距离敏感。通过将测量光谱与在B3LYP/6 - 311++G(3df,3pd)水平下为候选结构计算的光谱进行比较,确定了配合物的结构。还使用CAM - B3LYP泛函计算了结合能。在所有情况下,CH4均显示与金属的η(2)配位。m = 1的配合物在最低的C - H伸缩振动中,相对于自由CH4的对称伸缩振动,显示出370 cm(-1)(对于M = Co)和320 cm(-1)(对于M = Ni)的非常大的红移。它们采用C2v结构,重原子和相邻氢原子共面。m = 2的配合物红移略有减小,且为T形结构。对于n = 3的配合物,观察到了T形和等边(或准等边)结构。测量的光解离起始点以及低频C - H伸缩振动强度的显著降低意味着Ni(+)(CH4)2 - CH4的结合能值为2650 ± 50 cm(-1)。Co(+)(CH4)4配合物有两种低能结构,准四面体和扭曲的平面正方形,这导致了丰富的光谱。相比之下,对称的平面正方形Ni(+)(CH4)4配合物的振动光谱非常简单。

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