A new physical model and experimental measurements of copper interconnect resistivity considering size effects and line-edge roughness (LER)

G. Lopez, J. Davis, J. Meindl
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引用次数: 40

Abstract

A new closed-form effective resistivity (rhoeff) model as a function of line-edge roughness (LER), sidewall specularity p, and grain boundary scattering R is presented. There is improved physical insight to increasing resistivity than previous models. The model is validated against former simulation data and calibrated with electrical measurements of fabricated Cu interconnect test structures exhibiting an average of 14 nm LER for line widths ranging from 61 nm to 332 nm. Upon fitting the new model to experimental data, p and R are determined to be 0 and 0.79, respectively. The model is also used to interpret ITRS 2007 projections for local wire resistivity. ITRS projections for resistivity can only be achieved with very high quality interconnect structures that have nearly elastic sidewall collisions (p=0.95), low grain reflectivity (R=0.40), and no line edge roughness (LER=0nm). In fact, adding 6.0nm of LER increases rhoeff by ~20% for 2022 (11nm node). Finally, a projection with pessimistic values of p=0, R=0.5 and LER=1.0nm predicts an 87% greater rhoeff value than the ITRS 2007 projection for the 11 nm node.
考虑尺寸效应和线边粗糙度的铜互连电阻率物理模型及实验测量
提出了一种新的封闭有效电阻率(rhoeff)模型,该模型是线边缘粗糙度(LER)、侧壁镜面率p和晶界散射R的函数。与以前的模型相比,提高了对电阻率增加的物理洞察力。根据先前的仿真数据验证了该模型,并使用制备的Cu互连测试结构的电测量进行了校准,在61 nm至332 nm的线宽范围内,平均LER为14 nm。将新模型与实验数据拟合后,确定p和R分别为0和0.79。该模型还用于解释ITRS 2007对局部导线电阻率的预测。电阻率的ITRS预测只能在非常高质量的互连结构中实现,这些互连结构具有几乎弹性的侧壁碰撞(p=0.95),低颗粒反射率(R=0.40),并且没有线边缘粗糙度(LER=0nm)。事实上,增加6.0nm的LER将使2022年(11nm节点)的rhoeff提高约20%。最后,悲观值为p=0, R=0.5和LER=1.0nm的预测比ITRS 2007预测的11 nm节点的rhoeff值高87%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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