Effect of wafer thickness on sheet resistance during spike annealing

S. Catlett, J. Shepard
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Abstract

Temperature control requirements for Rapid Thermal Anneal (RTA) process steps, notably the source/drain activation anneal, have reached the limits of process capability at the 65 nm node. Device requirements dictate the tools be matched to better than 2°C and peak-temperature controlled to better than 1°C at ramp-up rates between 75°C/s and 230°C/s. It is important to understand all sources of variation in the time-temperature profile and the effects of this variation on measured parameters such as sheet resistance (Rs) on both monitor and product wafers. This work examines the effect of wafer thickness on the time-temperature behavior during the RTA process and its subsequent effect on Rs. It is shown that thicker wafers lead to a lower Rs. Nominal wafer thickness is 750 μm, but a variation in thickness of 10 μm results in an Rs shift of 0.5 ohms/square, the equivalent to a peak-temperature change of 0.63°C. This behavior is shown to have a significant effect on both monitor and product wafers. A study of 100 Hz data from the RTA chamber shows that this effect is likely due to two factors: (1) Thicker wafers reach a higher peak temperature, and (2) after reaching peak temperature, thicker wafers cool more slowly. Peak temperature reached is seen to change by 0.34°C per 10 μm of thickness change. The cooling rate changes by approximately 1°C/s per 10 μm of thickness change. Together, higher peak temperature and lower cooling rate result in a higher thermal budget, greater activation, and lower Rs for thicker wafers.
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尖峰退火过程中晶圆厚度对片材电阻的影响
快速热退火(RTA)工艺步骤的温度控制要求,特别是源/漏激活退火,已经达到65nm节点的工艺能力极限。设备要求工具匹配温度高于2°C,峰值温度控制在1°C以上,升温速率在75°C/s至230°C/s之间。重要的是要了解时间-温度曲线变化的所有来源,以及这种变化对测量参数的影响,如监视器和产品晶圆上的片材电阻(Rs)。本研究考察了晶圆厚度对RTA过程中时间-温度行为的影响及其随后对Rs的影响。结果表明,晶圆厚度越厚,Rs越低。公称晶圆厚度为750 μm,但厚度变化10 μm会导致Rs偏移0.5欧姆/平方,相当于峰值温度变化0.63°C。这种行为对显示器和产品晶圆都有显著的影响。对RTA腔室100 Hz数据的研究表明,这种影响可能是由于两个因素造成的:(1)较厚的晶圆达到更高的峰值温度;(2)在达到峰值温度后,较厚的晶圆冷却得更慢。厚度每变化10 μm,峰值温度变化0.34℃。厚度每变化10 μm,冷却速率约为1°C/s。更高的峰值温度和更低的冷却速率共同导致更高的热收支,更高的激活和更厚的晶圆更低的r。
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