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Negative ions of nitroethane and its clusters

机译:硝基乙烷及其簇的负离子

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Valence and dipole-bound negative ions of the nitroethane (NE) molecule and its clusters are studied using photoelectron spectroscopy (PES), Rydberg electron transfer (RET) techniques, and ab initio methods. Valence adiabatic electron affinities (EA(a)s) of NE, C2H5NO2, and its clusters, (C2H5NO2)(n), n=2-5, are estimated using vibrationally unresolved PES to be 0.3 +/- 0.2 eV (n=1), 0.9 +/- 0.2 eV (n=2), 1.5 +/- 0.2 eV (n=3), 1.9 +/- 0.2 eV (n=4), and 2.1 +/- 0.2 eV (n=5). These energies were then used to determine stepwise anion-neutral solvation energies and compared with previous literature values. Vertical detachment energies for (C2H5NO2)(n)(-) were also measured to be 0.92 +/- 0.10 eV (n=1), 1.63 +/- 0.10 eV (n=2), 2.04 +/- 0.10 eV (n=3), and 2.3 +/- 0.1 eV (n=4). RET experiments show that Rydberg electrons can be attached to NE both as dipole-bound and valence bound anion states. The results are similar to those found for nitromethane (NM), where it was argued that the diffuse dipole state act as a "doorway state" to the more tightly bound valence anion. Using previous models for relating the maximum in the RET dependence of the Rydberg effective principle number n(max)(*), the dipole-bound electron affinity is predicted to be similar to 25 meV. However, a close examination of the RET cross section data for NE and a re-examination of such data for NM finds a much broader dependence on n(*) than is seen for RET in conventional dipole bound states and, more importantly, a pronounced ... dependence is found in n(max)(*) (n(max)(*) increases with ...). Ab initio calculations agree well with the experimental results apart from the vertical electron affinity value associated with the dipole bound state which is predicted to be 8 meV. Moreover, the calculations help to visualize the dramatic difference in the distributions of the excess electron for dipole-bound and valence states, and suggest that NE clusters form only anions where the excess electron localizes on a single monomer.
机译:使用光电子能谱(PES),里德堡电子转移(RET)技术和从头算方法研究了硝基乙烷(NE)分子及其簇的价和偶极结合的负离子。 NE,C2H5NO2及其簇的(C2H5NO2)(n)的价绝热电子亲和力(EA(a)s,n = 2-5)使用振动未解析的PES估算为0.3 +/- 0.2 eV(n = 1),0.9 +/- 0.2 eV(n = 2),1.5 +/- 0.2 eV(n = 3),1.9 +/- 0.2 eV(n = 4)和2.1 +/- 0.2 eV(n = 5) )。然后将这些能量用于确定逐步的阴离子中性溶剂化能量,并将其与以前的文献值进行比较。 (C2H5NO2)(n)(-)的垂直脱离能也测得为0.92 +/- 0.10 eV(n = 1),1.63 +/- 0.10 eV(n = 2),2.04 +/- 0.10 eV(n = 3)和2.3 +/- 0.1 eV(n = 4)。 RET实验表明,Rydberg电子可以偶极结合和价键结合的形式附着在NE上。结果类似于在硝基甲烷(NM)上发现的结果,在该论据中,弥散偶极子态充当与更紧密结合的化合价阴离子的“门态”。使用以前的模型来关联里德堡有效原理数n(max)(*)的RET依赖性最大值,偶极子结合电子亲和力预计类似于25 meV。但是,仔细检查NE的RET横截面数据,再检查NM的这种数据,发现对n(*)的依赖性比常规偶极子束缚态中对RET的依赖性大得多,更重要的是, ...在n(max)(*)中发现依赖关系(n(max)(*)随着...的增加而增加)。从头算计算与实验结果非常吻合,除了与偶极子束缚态相关的垂直电子亲和力值(预计为8 meV)外。此外,这些计算有助于可视化偶极结合态和价态的过量电子分布的显着差异,并表明NE簇仅形成阴离子,其中过量电子位于单个单体上。

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