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On the growth dynamics of neutral vanadium oxide and titanium oxide clusters

机译:中性氧化钒和氧化钛团簇的生长动力学

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Cluster growth dynamics of vanadium oxide and titanium oxide clusters produced by laser ablation of vanadium and titanium metal in a He gas flow seeded with up to 2% O_2 are studied by covariance mapping time-of-flight mass spectrometry. Covariance mapping enables the recognition of two different distribution components in the overall homogeneous mass spectra for both vanadium oxide and titanium oxide cluster systems. The oxygen-rich component Or shows small correlated fluctuations while the oxygen-poor component Op shows large correlated fluctuations. These two cluster distribution components are observed at low ablation laser powers and low expansion gas concentrations. Fluctuations of small vanadium oxide clusters (V_2O, V_2O_2, and V_2O_3) and small titanium oxide clusters (Ti_2O_2 and Ti_2O_3) are covariance determining. The less fluctuating V_2O_3 and Ti_2O_3 clusters are "nuclei" for the oxygen-rich components Or. The more fluctuating V_2O and Ti_2O_2 are "nuclei" for the oxygen poor components Op. Correlated fluctuations or covariances within each distribution component are constant. Covariances for the different distribution components are different. Studies of mass spectra and covariances as functions of ablation laser power and expansion gas concentration imply that V_2O and Ti_2O_2 clusters are formed in different regions of the ablation plasma plume than V_2O_3 and Ti_2O_3. We suggest that V_2O_3 and Ti_2O_2 are formed in the colder plasma region farther away from the ablated metal surface. Larger vanadium oxide and titanium oxide clusters grow from these small clusters by very specific pathways which involve only uptake of VO or VO_2, and TiO_2, respectively.
机译:通过协方差映射飞行时间质谱研究了在2%O_2以内的He气流中激光烧蚀钒和钛金属产生的氧化钒和氧化钛簇的簇生长动力学。协方差映射可以识别钒氧化物和钛氧化物簇系统的整体均匀质谱中的两个不同分布成分。富氧组分Or显示较小的相关波动,而贫氧组分Op显示较大的相关波动。在低烧蚀激光功率和低膨胀气体浓度下观察到这两个簇分布分量。小钒氧化物簇(V_2O,V_2O_2和V_2O_3)和小钛氧化物簇(Ti_2O_2和Ti_2O_3)的涨落是协方差确定的。波动较小的V_2O_3和Ti_2O_3团簇是富氧组分Or的“核”。 V_2O和Ti_2O_2的起伏较大,是贫氧组分Op的“核”。每个分布分量内的相关波动或协方差是恒定的。不同分布分量的协方差是不同的。质谱和协方差作为烧蚀激光功率和膨胀气体浓度的函数的研究表明,与V_2O_3和Ti_2O_3相比,V_2O和Ti_2O_2团簇形成在烧蚀等离子体羽的不同区域。我们建议在更冷的等离子体区域中形成V_2O_3和Ti_2O_2,该区域离烧蚀的金属表面更远。较大的钒氧化物和钛氧化物簇通过非常特定的途径从这些小簇中生长出来,这些途径仅分别吸收VO或VO_2和TiO_2。

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