Skip to main content Accessibility help
  • Print publication year: 2010
  • Online publication date: July 2014

14 - Stress migration in thin films



Stress-induced atomic migration is creep as we have discussed in Chapter 10. We have emphasized that it is stress gradient not stress that can induce atomic diffusion. From the viewpoint of device reliability, we must ask the following questions. First, from where is the stress coming? Second, how does a stress gradient develop in an interconnect? Third, how can the elastic stress gradient induce atomic migration? Fourth, what is the mechanism of creep that leads to void or whisker formation to cause failure in interconnects? Finally what is the rate of creep [1–4]?

On the first question, typically the answer is thermal stress which occurs due to different thermal expansion coefficients in the interconnect structure. The most obvious one is that between Al (or Cu) metallic wire and the interlayer dielectric insulator. Another one comes from the chip-packaging interaction in flip-chip technology because of the large difference in thermal expansion between the chip and the packaging substrate. Then, electromigration can introduce back-stress in interconnects as discussed in Chapter 11, Section 11.6. Mechanical stress due to externally applied force is rare in electronic devices. However, we should mention impact-induced stress due to the dropping of a handheld device to the ground. The impact is a high rate shear in a very short time, about 1 millisecond, or a shear rate of 1 × 103 cm/s. Since impact failure is not a long-time event as in creep, we will not cover it here.

[1] C., Herring, “Diffusional viscosity of a polycrystalline solid,” J. Appl. Phys. 21 (1950), 437.
[2] B., Chalmers, Physical Metallurgy (Wiley, New York, 1959).
[3] A. S., Nowick and B. S., Berry, Anelastic Relaxation in Crystalline Solids (Academic Press, New York, 1972).
[4] M. F., Ashby and D. R. H., Jones, Engineering Materials I (Pergamon Press, Oxford, 1980).
[5] Fan-Yi, Ouyang, Kai, Chen, K. N., Tu and Yi-Shao, Lai, “Effect of current crowding on whisker growth at the anode in flip chip solder joints,” Appl. Phys. Lett. 91 (2007), 231919.
[6] K. N., Tu, “Interdiffusion and reaction in bimetallic CuSn thin films,” Acta Met. 21 (1973), 347.
[7] K. N., Tu and R. D., Thompson, “Kinetics of interfacial reaction in bimetallic CuSn thin films,” Acta Met. 30 (1982), 947.
[8] K. N., Tu, “Irreversible processes of spontaneous whisker growth in bimetallic CuSn thin film reactions,” Phys. Rev. B49 (1994), 2030–4.
[9] G. T. T., Sheng, C. F., Hu, W. J., Choi, K. N., Tu, Y. Y., Bong and Luu, Nguyen, “Tin whiskers studied by focused ion beam imaging and transmission electron microscopy,” J. Appl. Phys. 92 (2002), 64–9.
[10] W. J., Choi, T. Y., Lee, K. N., Tu, N., Tamura, R. S., Celestre, A. A., MacDowell, Y. Y., Bong and L., Nguyen, “Tin whisker studied by synchrotron radiation micro-diffraction,” Acta Mat. 51 (2003), 6253–61.