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1 - Erich Schmid Institute

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C.3 Discussion and Concluding Remarks<br />

from the deflection versus film thickness-curve as depicted in Fig.C.6 for three examples.<br />

The characteristic of such a curve allows the estimation of the stress profile because the<br />

actual deflection correlates directly with the stresses in the sublayer removed. After having<br />

removed the thin film in a section, the deflection has a predictable value which comes<br />

solely from the curved indicator, because the substrate is stress free and straight. Since<br />

this deflection is equal for all sections, it gives further information about the accuracy<br />

of the experiment. The sign of the stress in the thin film removed can be estimated<br />

simply from the change of the deflection at the interface (tf = 0µm). A drop indicates<br />

tensile stresses, whereas an increase of the deflection leads to the conclusion that the<br />

stress removed was compressive.<br />

Figure C.6: Examples of measured deflections versus film thickness. The drops of the measured deflections<br />

after having removed the thin film and the diffusion barrier (db) completely in<br />

sections A2 and A3 indicate tensile film stresses. In section A9, the film was subjected to<br />

compressive stresses which leads to an increase of the deflection.<br />

In summary, the presented 3D-ILR method is a powerful tool to determine two- and<br />

three-dimensional stress profiles in surface near layers. The direct approach and the<br />

simple calculation procedure make it a good choice for the evaluation of such stress<br />

distributions with a depth resolution on a nanoscale and a lateral resolution on a micron<br />

scale.<br />

C–7<br />

C

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