“…An interlayered dielectric material in a device is commonly interfaced to itself as well as a number of other materials such as silicon, silicon nitride, silicon oxide, aluminum, copper, chromium, tungsten, capping metals, and ceramic. In general, residual stress at an interface arises from a drastic difference in the physical properties of the interfaced layers (namely, thermal expansion coefficient, Young's modulus, and Poisson's ratio), and is further influenced by thermal history [16][17][18]. The residual stress, associated mainly with thermal mismatches, can be reduced by adjusting the properties of interfaced layers and optimizing the heat-treatment process.…”