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Time-resolved mass and energy spectral investigation of a pulsed polymerising plasma struck in acrylic acid

机译:在丙烯酸​​中撞击的脉冲聚合等离子体的时间分辨质量和能谱研究

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摘要

This paper details an electrical diagnostic study of the discharge used in the pulsed plasma polymerisation of acrylic acid. The capacitively coupled RF discharge was operated at a frequency of 1 kHz and a pressure of 1.3 Pa. Using a retractable deposition-protected Langmuir probe the time-resolved electron temperature, density and plasma potential in the bulk were obtained. The time-resolved ion energy distribution functions (IEDFs) relative to ground potential for a selection of masses (m/z = 19, 55, 73) and the mass spectra (2-100 amu) have been measured by the energy-resolved mass spectrometer using an improved double gating technique. In both the "on" and "off" times of the pulse, the IEDFs for the heavier mass ions are characterised by a single peak (E-p - hereafter - the energy which corresponds with the peak intensity), the position and width of which are determined by the time-dependent plasma potential VP and its distribution across the plasma to the spectrometer, while a weakly bimodal ion energy distribution is present in the IEDF for m/z= 19 in the "on" time. In the steady "on" time, the relative ion flux (detector count rate) of each species and the energy corresponding to the peak intensity in the IEDFs are constant, the latter (E-p similar to 47 eV) correlating very well to the probe measured plasma potential. At pulse initiation, V-p rises to values > 90 V, however, these energies are not detected in IEDF with our time resolution of 10 mu s. In the "off" time, this energy falls with a two-fold decay time, initially sharply to similar to 23 eV (at the first measured point which was made 1 mu s after beginning of the "off" period) and then slowly in the next 150 mu s to similar to 17-18 eV closer to the end of the cycle. The elevation of the E-p well above ground is in contrast to that usually observed in pulsed Ar discharges (similar to 10 V higher), due to in this case, charging of the acrylic acid deposited materials on the walls. The time-history of the integrated area under the IEDFs reveals that after the initiation of the "on" time the concentration N of lighter species rises more quickly than the heavier ones. In the "off" time, however, although N-19 becomes negligible after 50 mu s, N-73 decreases more quickly than N-55 which is still non-zero at 150 mu s. The time resolved mass-spectral reveal the general mass dependency in the concentration rise and fall times of the detected species. (c) 2005 Elsevier B.V. All rights reserved.
机译:本文详细介绍了丙烯酸脉冲等离子体聚合中使用的放电的电诊断研究。电容耦合RF放电在1 kHz的频率和1.3 Pa的压力下运行。使用可伸缩的沉积保护型Langmuir探针,可以测量主体中时间分辨的电子温度,密度和等离子体电势。相对于地面电势的时间分辨离子能量分布函数(IEDFs)通过能量分辨质量测量了质量选择(m / z = 19、55、73)和质谱图(2-100 amu)光谱仪使用改进的双选通技术。在脉冲的“开”和“关”时间内,重离子的IEDF都具有一个峰(Ep-此后为与峰强度对应的能量),其位置和宽度分别为由时间相关的等离子电势VP及其在整个等离子至光谱仪中的分布确定,而IEDF中在“开启”时间内m / z = 19时存在弱双峰离子能量分布。在稳定的“接通”时间内,每种物质的相对离子通量(检测器计数率)和对应于IEDF中峰值强度的能量是恒定的,后者(Ep类似于47 eV)与测得的探针具有很好的相关性血浆电势。在脉冲启动时,V-p上升到> 90 V的值,但是,在我们的时间分辨率为10 s的IEDF中,未检测到这些能量。在“关闭”时间中,该能量以两倍的衰减时间下降,最初急剧下降至类似于23 eV(在“关闭”时间段开始后1 s的第一个测量点),然后缓慢下降。接下来的150μs接近周期结束时接近17-18 eV。 E-p高出地面的高度与通常在脉冲Ar放电(大约高10 V)中观察到的高度相反,这是因为在这种情况下,壁上丙烯酸沉积材料的电荷增加。 IEDFs下整合区域的时间历史表明,在“开启”时间开始后,较轻物种的浓度N升高得更快。但是,在“关闭”时间内,尽管N-19在50 s s后可以忽略不计,但N-73的下降速度要快于在150 s s仍非零的N-55。时间分辨质谱揭示了检测到的物种浓度上升和下降时间的一般质量依赖性。 (c)2005 Elsevier B.V.保留所有权利。

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