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首页> 外文期刊>Vacuum: Technology Applications & Ion Physics: The International Journal & Abstracting Service for Vacuum Science & Technology >Studies of co-implanted helium and hydrogen with an intermediate annealing step for thermal splitting of bonded silicon to oxide-coated wafers
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Studies of co-implanted helium and hydrogen with an intermediate annealing step for thermal splitting of bonded silicon to oxide-coated wafers

机译:用中间退火步骤研究共注入氦和氢,以将键合硅热分裂成氧化膜晶圆

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Layer transfer by thermal or mechanical splitting of implanted silicon wafers can often require processing at elevated temperatures before bonding and annealing. The possibility has been investigated here of making two implants, the first defining a damage plane for splitting, the second being made after high-temperature processing. Helium and hydrogen implanted wafers were annealed at various temperatures, T-a, this being followed by a second implantation of either gas. Thermal splitting of bonded wafer pairs was studied for both implants to the same projected range, R-p, and with hydrogen implanted to R-p = 25% less than helium. In the former case, complete thermal splitting occurred for T-a less than or equal to 550 degreesC; for T-a > 550 degreesC, wafers failed to split or delaminated at the bond interface. When hydrogen was implanted to a shallower depth complete thermal splitting occurred for T-a less than or equal to 500 degreesC. The split occurred at the hydrogen R-p for T-a < 400 degreesC and at the helium R-p for T-a = or > 400 degreesC. Above T-a = 500 degreesC a decreasing percentage of the total silicon area was transferred. At 400 degreesC measurements suggested that splitting occurred at both helium and hydrogen R-p planes and it is believed that helium platelet formation at this temperature is an important factor. For T-a < 400 degreesC, helium, a proportion of which may have diffused towards the peak of the hydrogen distribution, is believed to react and produce splitting there during bond-annealing. For T-a > 400 degreesC, sufficient hydrogen is thought to diffuse during bond-annealing towards the peak of the helium distribution and react there to produce the weakest splitting plane. For T-a > 500 degreesC, loss of helium, annealing out of strain and break-up of platelets into bubble-cavities reduces the probability of thermal splitting. When hydrogen was implanted first, complete thermal splitting occurred for T-a less than or equal to 300 degreesC but was inconsistent at 400 degreesC and above. (C) 2004 Elsevier Ltd. All rights reserved.
机译:通过热或机械分裂注入的硅晶片而进行的层转移通常可能需要在键合和退火之前在升高的温度下进行处理。这里研究了制造两种植入物的可能性,第一种植入物确定了用于分裂的损伤平面,第二种植入物是在高温处理之后制成的。氦和氢注入的晶片在不同的温度T-a下退火,然后再注入两种气体。研究了两种植入物在相同的投射范围R-p下键合晶片对的热分裂,氢注入到R-p上比氦气少25%。在前一种情况下,T-a小于或等于550摄氏度时发生了完全热分裂;当T-a> 550°C时,晶圆无法在键合界面处分裂或分层。当将氢注入到较浅的深度时,T-a小于或等于500摄氏度时会发生完全热分裂。对于T-a <400摄氏度,氢原子R-p发生分裂;对于T-a =或> 400摄氏度,氦气R-p发生分裂。在T-a = 500℃以上,转移了总硅面积的递减百分比。在400℃下的测量表明,在氦和氢R-p平面上均发生分裂,并且据信在此温度下氦血小板的形成是重要的因素。对于T-a <400摄氏度,据信在键合退火过程中氦(其中一部分可能已向氢分布的峰值扩散)会发生反应并在此处产生分裂。对于T-a> 400摄氏度,认为在键合退火过程中有足够的氢向氦分布的峰值扩散,并在那发生反应以产生最弱的分裂面。对于T-a> 500摄氏度,氦气的损失,应变的退火以及血小板破裂成气泡的可能性降低了热分裂的可能性。当首先注入氢时,T-a在小于或等于300摄氏度时发生完全热分裂,但在400摄氏度或更高温度下不一致。 (C)2004 Elsevier Ltd.保留所有权利。

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