用x射线法测量溅射Cu薄膜残余应力分布

Y. Akiniwa, H. Kimura, Takuhisa Sakaue
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摘要

采用射频磁控溅射法制备了三种铜薄膜。选择10和150W的目标功率来改变薄膜的性能。薄玻璃片被用作衬底。当目标功率为150W时,沉积时间分别为7和40min。厚度分别为0.6μm和2.9μm,测得的晶粒尺寸分别为243nm和450nm。较厚薄膜的晶粒尺寸大于较薄薄膜。另一方面,当目标功率为10W时,厚度为2.4μm,晶粒尺寸为54nm。晶粒尺寸也取决于目标功率。用x射线法测量了薄膜的残余应力分布。采用了掠入射x射线衍射法、等穿透深度法和传统的sin2ψ法。实测加权平均应力随深度增加而增大。在距地表约0.3μm处达到最大值后,随深度增加而减小。在150W下沉积的薄膜中,近表面的应力分布几乎相同,与厚度无关。另一方面,当目标功率为10W时,应力分布向压缩侧偏移。其原因可以用热残余应力的影响来解释。利用优化技术估计了实际应力分布。应力在距表面0.5μm处达到最大值,靠近基体处为压应力。
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Measurement of Residual Stress Distribution in Sputtered Cu Thin Films by X-Ray Method
Three kinds of copper thin films were fabricated by RF-magnetron sputtering. The target power was selected to be 10 and 150W to change the properties of the films. Thin glass sheet was used as a substrate. For the target power of 150W, the deposition time was selected to be 7 and 40min. The thickness was 0.6μm and 2.9μm, and the grain size measured was 243nm and 450nm, respectively. The grain size of thicker film was larger than that of thinner one. On the other hand, for the target power of 10W, the thickness and grain size were 2.4μm and 54nm, respectively. The grain size depends on the target power, too. The residual stress distribution in the films was measured by X-ray method. Several methods such as the grazing incidence X-ray diffraction method, the constant penetration depth method and the conventional sin2ψ method were adopted. The measured weighted average stress increased with increasing depth. After taking the maximum value at about 0.3μm from the surface, the value decreased with increasing depth. The stress distribution near the surface in the films deposited at 150W was almost identical irrespective of thickness. On the other hand, for the target power of 10W, the stress distribution shifted to compression side. The reason could be explained by the effect of the thermal residual stress. The real stress distribution was estimated by using the optimization technique. The stress took the maximum value at 0.5μm from the surface, and was compressive near the substrate.
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