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Dynamics and Interaction of Active Centers at Nanocarbon Electron Emitters

机译:纳米碳电子发射器活性中心的动态与相互作用

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Enhanced electron field-induced emission from layers composed by nanocarbon low-aspect-ratio (i.e. not very elongated) particles still doesn't have complete theoretic explanation. Our previous experimental results [1,2] indicated that this phenomenon can be possibly attributed to the effect of non-stationary electric field component associated with kHz- or MHz-frequency current fluctuations. "Non-conservative" rf field action in a heterogeneous system can affect electron energy distributions thus facilitating extraction of electrons into vacuum. This work was aimed to demonstrate presence of rf field and investigate properties of field-induced emission current fluctuations with spatial resolution. The presented early experiments were performed with a strongly non-uniform sample of nanoporous carbon (NPC, [3]) using the scheme and techniques described in detail in [4]. The sample produced full emission current up to 20μA for 12-18 kV dc voltage applied to 2.5 mm-wide cathode-anode gap. Comparison of area-resolved current density waveforms and their frequency spectra obtained for different probe positions revealed a few possible types of current fluctuations' scenarios. For some of the emission image spots, averaged spectra were almost uniform, similar to "white noise" frequency distributions (curve 1 in Fig. 1). Though, the corresponding current waveforms, being disordered over the most part of their length, included intervals of periodic and even quasi-harmonic modulation. At other probe positions, relatively low-frequency components (below 100 kHz) prevailed in the oscillatory spectra, as it is showed by curve 2 in Fig. 1. Low-current-density signals often had the form of a succession ofμs-long "bursts" with falls practically to zero level in pauses between them.
机译:增强由纳米碳宽高比(即不是非常细长)颗粒组成的层的电子场诱导的发射仍然没有完整的理论解释。我们以前的实验结果[1,2]表明这种现象可能归因于与KHZ或MHz频率电流波动相关的非静止电场分量的效果。异构系统中的“非保守”RF场动作可以影响电子能量分布,从而促进电子进入真空。这项工作旨在证明RF场的存在,并调查具有空间分辨率的现场诱导的发射电流波动的特性。使用[4]中详细描述的方案和技术,用强烈不均匀的纳米多孔碳(NPC,[3])进行呈现的早期实验。将样品产生高达20μA的完全发射电流,用于12-18 kV DC电压,施加到2.5mm宽的阴极 - 阳极间隙。区域分辨电流密度波形的比较及其对不同探针位置获得的频谱揭示了几种可能类型的电流波动的场景。对于一些发光图像斑点,平均光谱几乎是均匀的,类似于“白色噪声”频率分布(图1中的曲线1)。虽然,相应的电流波形,在其长度的大部分大部分中,包括周期性甚至准谐波调制的间隔。在其他探针位置,在振荡谱中,在振荡谱中占相出的相对低频分量(低于100kHz),因为它通过图1中的曲线2表示。低电流密度信号通常具有μs长的连续形式的形式“突发“几乎跌落到它们之间的暂停中的零水平。

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