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首页> 外文期刊>The journal of physical chemistry, A. Molecules, spectroscopy, kinetics, environment, & general theory >The Arsenic Fluorides AsF_n (n = 1-6) and Their Anions: Structures, Thermochemistry and Electron Affinities
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The Arsenic Fluorides AsF_n (n = 1-6) and Their Anions: Structures, Thermochemistry and Electron Affinities

机译:氟化砷AsF_n(n = 1-6)及其阴离子:结构,热化学和电子亲和力

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摘要

The molecular structures, electron affinities, and dissociation energies of the AsF_n/AsF_n~- (n = 1-6) species have been examined using four hybrid and pure density functional theory (DFT) methods. The basis set used in this work is of double-ζ plus polarization quality with additional diffuse s- and p-type functions, denoted DZP++. The geometries are fully optimized with each DFT method independently. Three types of energy separations reported in this work are the adiabatic electron affinity (EA_ad), the vertical electron affinity (EA_vert), and the vertical detechment energy (VDE). The first As-F dissociation energies D_e(F_(n-1)As-F) for AsF_n, and both D_e(F_(n-1)As~--F) and D_e(F_(n-1)As-F~-) species have also been reported. The best method for predicting molecular structures was found to be BHLYP, while other methods generally overestimated bond lengths. For the closed-shell anions the As-F bond distances are ~0.1 A longer than those for the analogous neutrals. In contrast, when the neutral AsF_n is a closed shell, the anion As-F distances is ~0.2 A longer. The most reliable adiabatic electron affinities, obtained at the DZP++BHLYP level of theory, are 0.74 eV (As), 0.94 eV (AsF), 1.17 eV (AsF_2), 0.80 eV (AsF_3), 4.42 eV (AsF_4), and 2.79 eV (AsF_5), respectively. Those for As and AsF_2 are in good agreement with experiment, but that for AsF is smaller than the available experimental value (1.3 ± 0.1 eV). The predicted vertical detachment energy for AsF_6~- is remarkable, as large as 10.54 eV (BHLYP), indicating AsF_6~- is stable. The general trend for predicting the first dissociation energies is BP86 ~ BLYP > B3LYP BHLYP. The first dissociation energies for the neutral arsenic fluorides predicted by the DFT methods except BHLYP are 4.22-4.5 eV (AsF), 4.45-4.74 eV (AsF_2), 4.76-5.03 eV (AsF_3) 1.46-1.84 eV (AsF_4), and 3.87-4.11 eV (AsF_5). Compared to the experimental dissociation energies, the theoretical predictions are very reasonable. The anion bond dissociation energies are largely unknown experimentally. The dissociation energy for AsF~- → As + F~- is predicted to be 1.73 eV (BHLYP), 1.82 eV (B3LYP), 1.93 eV (BP86), and 1.87 eV (BLYP), which values are in good agreement with experiment (1.92 ± 0.2 eV). The predicted bond dissociation energies for D_e(F_3As-F~-) are in the range of 2.45-2.57 eV, which is close to the previous theoretical results using the HF and MP2/ECP methods. For the vibrational frequencies of the AsF_n series, the BHLYP method also produces good predictions with the average error only about 10 cm~(-1) from available experimental values. The other three methods underestimate the vibrational frequencies, with the worst predictions given by the BLYP method.
机译:使用四种混合和纯密度泛函理论(DFT)方法研究了AsF_n / AsF_n〜-(n = 1-6)物种的分子结构,电子亲和力和解离能。在这项工作中使用的基础集是双ζ加上极化质量以及附加的扩散S和P型函数,表示为DZP ++。每种DFT方法都对几何形状进行了完全优化。这项工作中报告的三种能量分离类型是绝热电子亲和力(EA_ad),垂直电子亲和力(EA_vert)和垂直分解能量(VDE)。 AsF_n的第一个As-F解离能D_e(F_(n-1)As-F)以及D_e(F_(n-1)As〜-F)和D_e(F_(n-1)As-F 〜-)种也有报道。发现预测分子结构的最佳方法是BHLYP,而其他方法通常会高估键长。对于闭壳阴离子,As-F键距比类似中性离子的键距长约0.1A。相反,当中性AsF_n为封闭壳时,阴离子As-F的距离要长〜0.2A。在DZP ++ BHLYP理论水平上获得的最可靠的绝热电子亲和力为0.74 eV(As),0.94 eV(AsF),1.17 eV(AsF_2),0.80 eV(AsF_3),4.42 eV(AsF_4)和分别为2.79 eV(AsF_5)。 As和AsF_2的那些与实验非常吻合,但是AsF的那些小于可用的实验值(1.3±0.1 eV)。 AsF_6〜-的预测垂直脱离能非常显着,高达10.54 eV(BHLYP),表明AsF_6〜-是稳定的。预测第一离解能的一般趋势是BP86〜BLYP> B3LYP BHLYP。用DFT方法预测的除BHLYP以外的中性氟化砷的第一离解能为4.22-4.5 eV(AsF),4.45-4.74 eV(AsF_2),4.76-5.03 eV(AsF_3)1.46-1.84 eV(AsF_4)和3.87 -4.11 eV(AsF_5)。与实验离解能相比,理论预测是非常合理的。阴离子键解离能在很大程度上是实验未知的。 AsF〜-→As + F〜-的离解能预计为1.73 eV(BHLYP),1.82 eV(B3LYP),1.93 eV(BP86)和1.87 eV(BLYP),这些值与实验吻合良好(1.92±0.2 eV)。 D_e(F_3As-F〜-)的预测键解离能在2.45-2.57 eV的范围内,这与使用HF和MP2 / ECP方法的先前理论结果相近。对于AsF_n系列的振动频率,BHLYP方法也产生了良好的预测,与可用的实验值相比平均误差仅为10 cm〜(-1)。其他三种方法低估了振动频率,而BLYP方法给出的预测最差。

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