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Architecture of RF Plasma Reactors

机译:射频等离子体反应器的架构

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In order to achieve a complete understanding and ocntrol of plasma processes an appropriate knowledge of the structure of the particular glow discharge utilized is necessary. This is extremely important because the electrical potention inside a plasma reactor is not uniform and therefore, as a function of the reactor geometry and sample position, charged particles are accelerated from the plasma bulk to the substrate to be treated by different potential drops, i.e. they impinge on different surface with different eneryg. As it willb e extensively shown in this book of proceedings, the charged particle bombardment (by positive ions, in particular), along with the nature of the materals exposed to the glow, play a key role in most treatments and deposition processes and hence the electrical staturs of the sample surface and of the other parts of the materials exposed to the glow, play a key role in most treatments and deposition processes and hence the leectrical status of the sample surface and of the other parts of the reactor have to be always evaluated. An example pertinent with the contents of this NATO-ASI, is the plasma assisted deposition of luoropolymers in fluorocarbon fed glow discharges. It has been reported(1,2), that ion bombardment increases the polymerization rate as well as the crosslinking and the inorganic characteristi of deposited polymer, but if the usbstrate potential is too negative with resppect to the plasma bulk, the ion bombardment is extremely endrgietic and causes a reduction of the polymerization rate or a complete stop of deposition. I nthese conditions hard-like carbon films instead of fluoropolymers are obtaned(3). A suitable combination of ion bombardment and of materials exposed to the plasma can influence the quali-quantitative composition of the plasma and therefore can sometime be utilized to improve the process performances. This expedient is very often utilized in dry etching of silicon oxide in fluorocarbon plasma for microelectronics applications. In orfer to reduce drastically the plasma concentration of flurorine atoms and to achieve the needed etch rate selectrivity with respect to silicon and/or silicon nitride, some parts of the reactor, subjected to intense and energetic ion bombardment, are made of silicon. The rapid and quantitative reaction between silicion and fluorine, under the synergistic effect of ion bombardment, drastically and increases the effect of CFx radicals (oxide etchants) mproving the process selectivity. Very negative potentials, on the othe rhand, must be avoided on those parts of the reactor whic can be easily sputtered and release unwanted species in the gas phase (e.g. stainless steel, aluminium, etc.) which contaminate the surface of the sample to be treated.
机译:为了获得对等离子体过程的全面理解和控制,必须充分了解所用特定辉光放电的结构。这一点非常重要,因为等离子反应器内部的电势不均匀,因此,根据反应器的几何形状和样品位置,带电粒子会通过不同的电位降从等离子体加速到要处理的基材,即它们用不同的eneryg撞击在不同的表面上。正如本书将在本书中广泛显示的那样,带电粒子轰击(尤其是正离子的轰击)以及暴露在辉光下的物质的性质在大多数处理和沉积过程中都起着关键作用,因此,样品表面和暴露在辉光下的材料的其他部分的电饱和度在大多数处理和沉积过程中起着关键作用,因此,样品表面和反应器其他部分的电气状态必须始终保持评估。与该NATO-ASI的内容有关的一个例子是在氟化碳进料的辉光放电中等离子体辅助的含氟聚合物的沉积。据报道(1,2),离子轰击提高了聚合速率以及沉积聚合物的交联性和无机特性,但如果等离子体势能相对于母体电位太负,则离子轰击会非常严重会产生不良影响,并导致聚合速率降低或沉积完全停止。在这种情况下,会变成硬状碳膜而不是含氟聚合物(3)。离子轰击和暴露于等离子体的材料的适当组合会影响等离子体的定性成分,因此有时可以用来改善工艺性能。该方法非常常用于微电子应用的碳氟化合物等离子体中的氧化硅干法蚀刻中。为了显着降低氟尿嘧啶原子的等离子体浓度并实现相对于硅和/或氮化硅的所需蚀刻速率选择性,反应器的某些部分受到了强烈的高能离子轰击,由硅制成。硅离子与氟之间的快速定量反应在离子轰击的协同作用下急剧地增加了CFx自由基(氧化物蚀刻剂)的作用,从而提高了工艺选择性。必须避免在反应堆的其他部分上产生非常负的电势,因为这些部分很容易溅射并释放出气相中不想要的物质(例如不锈钢,铝等),这些物质污染了待测样品的表面。治疗。

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