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首页> 外文期刊>International journal of mass spectrometry >Thermally activated decay channels of superhot C_(60)~-: delayed electron emission and dissociative attachment studied by hyperthermal negative surface ionization
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Thermally activated decay channels of superhot C_(60)~-: delayed electron emission and dissociative attachment studied by hyperthermal negative surface ionization

机译:超热C_(60)〜-的热激活衰变通道:延迟负电子发射和离解性附着的高温负电离研究

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摘要

Superhot C_(60)~- ions were formed by attachment of low energy free electrons to superhot C_(60)~0 molecules in effusive beam. We have studied the thermally activated decay of the C_(60)~- ion as a function of its vibrational temperature. In addition to the main channel of delayed electron emission C_(60)~- -> C_(60)~0 + e~-, we give evidence for a secondary channel (only weakly competitive) of dissociative attachment C_(60)~0 + e~- ->C_(58)~0 + C_2~-. We have found no evidence for the nearly isoenergetic complementary channel C_(60)~0 + e~- -> C_(58)~- + C_2~0. In order to measure the initial C_(60)~- beam flux (which partially decays to C_(60)~0 during the flight time) independently for each nozzle temperature we have used a unique detection method that is completely insensitive to the initial charge state and therefore to the ratio of charge states in the primary beam. The method is based on collisional electron exchange and negative ion (C_(60)~-) formation in a hyperthermal collision with a surface. Analyzing the kinetics of the delayed electron emission we have obtained a straight Arrhenius plot with a slope (activation energy) of 2.64 +- 0.07 eV and intersection (A value) of 1.3 * 10~(11) s~(-1). This value of the pre-exponential factor is in good agreement with former measurements but is several orders of magnitude lower than current models' predictions. A possible explanation for this difference is discussed.
机译:超热C_(60)〜-离子是通过将低能自由电子附着到喷流束中的超热C_(60)〜0分子上而形成的。我们研究了C_(60)〜-离子的热活化衰减随其振动温度的变化。除了延迟电子发射的主要通道C_(60)〜-> C_(60)〜0 + e〜-,我们还提供了解离附件C_(60)〜0的辅助通道(仅弱竞争性)的证据。 + e〜--> C_(58)〜0 + C_2〜-。我们没有发现几乎等能量的互补通道C_(60)〜0 + e〜--> C_(58)〜-+ C_2〜0的证据。为了分别测量每个喷嘴温度的初始C_(60)〜-光束通量(在飞行过程中部分衰减为C_(60)〜0),我们使用了一种对初始电荷完全不敏感的独特检测方法状态,因此与主光束中的电荷状态比率有关。该方法基于碰撞电子交换和在与表面的高温碰撞中形成负离子(C_(60)〜-)。分析延迟电子发射的动力学,我们获得了一条直线的Arrhenius图,其斜率(激活能)为2.64±0.07 eV,交点(A值)为1.3 * 10〜(11)s〜(-1)。前指数因子的值与以前的测量值非常吻合,但比当前模型的预测值低几个数量级。讨论了这种差异的可能解释。

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