Al薄膜金属化的热-机械循环行为

H. Hieber, T. Simon
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引用次数: 2

摘要

铝基薄膜金属化被用作集成电路和大多数分立有源元件的电气互连[1]。通过蒸发或溅射在400 - 450K的温度下沉积后,对金属化层进行不同的热处理:在T- 320K的温度下进行光阻剂的烘烤和离子蚀刻,在T- 720k的温度下与Si进行欧姆接触的合金化,在T- 500k的温度下进行模具粘合和热超声丝粘合,在T- 430k的温度下进行封装成型。在生产步骤完成后,组件将在T>520K的印刷电路板上进行软焊,并在T- 220k至T=500K之间进行热循环。在指定温度下的时间步长范围在几到103秒之间,热速率高达T102Ks-1。由于薄膜厚度h'1i,晶粒尺寸d.,5pm以及晶格缺陷的浓度,热处理引起了薄膜结构和局部化学成分的变化。由于薄膜和硅片具有不同的热膨胀系数aF和cr。基材比薄膜厚得多,机械刚性也更强,薄膜受到热压缩或拉伸应变。诱导应力超过薄膜的屈服点。从扩散蠕变[2]、位错滑移[13]和比较作用于移动晶界和晶粒空位的不同驱动力[4]来解释金属薄膜在T连续变化过程中的张力松弛。层错能低的金属晶粒生长不连续[5]。铝基薄膜表现出丘状的形成[6,7],这还没有定量地解释。本文的目的是通过对热处理过程中应力松弛的测量,了解基底上al基金属化薄膜中部分可逆和不可逆缺陷反应机理的动力学。结果表明,扩散蠕变和单晶粒生长的顺序与热、力学历史密切相关。直流电阻的变化表明在拉伸应力下晶格缺陷的产生和压缩应力下的吸收。初始晶粒尺寸为(100…透射电镜截线测量溅射膜的蒸发厚度为300 nm,溅射膜厚度为(1 ~ 3)nm。膜内横向宏观应力>1。通过化学蚀刻去除铝膜前后的衬底曲率测量了300K时的OMPa。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Thermo-Mechanical Cycling Behavior of Al Thin-Film Metallization
Al-based thin-film metallizations are used as electrical interconnections in integrated circuits and in most of discrete, active components L1]. After deposition at temperatures T between 400 and 450K by evaporat ion or sputtering, different thermal treatments work on the metallizations: The baking of photoresists and the ion etching upto T 320K, the alloying of ohmic contacts with Si upto T-720K, the die bonding and the thermosonic wire bonding at T-500K, the moulding of the encapsulation at T-430K. After the production steps the components are subject to softsoldering on printed-circuit boards with T>520K and thermal cycling during the application between T-220K and T=500K. The time st eps at the named temperatures range between few and 103s, the thermal rates get up to T102Ks-1. Due to the filmn thickness h'1i, the grain sizes d.,5pm and the concentration of lattice defects the thermal treatments cause changes in the film structure and local chemical composition. As the filrns and Si wafers have different coefficients of thermal expansion aF and cr.,.and the substrates are much thicker and mechanically rnore rigid than the films, the films are subjected to thermal compressive or tensile strains. The induced stresses exceed the yield point of the films. The straln relaxation of the metal films during continuous changes in T is explained in terms of diffusional creep [2], of dislocation slip [13] and by comparison of the different driving forces working on mobile grain boundaries and vacancies in the grains [4]. Metals with low stacking fault energy show discontinuous grain growth [5]. Al-based films exhibit the formation of hillocks [6,7] which is not yet explained quantitatively. The purpose of this paper is to learn the kinetics of partially reversible and of irreversible defect reaction mechanisms in Al-based thin-film metallizations on substrates from the measurement of stress relaxation during thermomechanical treatments. It will be shown that the sequence of diffusional creep and of the growth of single grains are sensitively dependent on the thermal and mechanical history. Changes in dc resistance indicate the production of lattice defects under tensile stress and the absorption under compressive stress. initial grain sizes are (100.. . 300)nm of the evaporated and (1...3)pm foir the sputtered films measured by line interception of TEM micrographs. The lateral macrostresses in the films are >1.OMPa at 300K measured by the substrate curvature before and after the removal of the Al films by chemical etching.
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