“…This is in Table 1 Experiment procedure of cyclic aging and annealing of gold films. 1 NP TH NP TH TH NP TH TH NP TH TH TH NP TH TH TH TH accordance with the literature that twins are seen frequently in gold thin films due to low stacking fault energy [16]. Ignoring the twin boundaries, an irregular column structure can be clearly seen.…”
Section: Resultssupporting
confidence: 87%
“…The same effect can also be used to explain the tensile stress generation during post-deposition annealing. Miller [14e16] indicated that defect annihilation was the reason for tensile stress generation caused by annealing in a limited regime (T < 125 C) [15,16]. The SEM and STEM micrographs revealed that an abundance of defects exist in the as deposited gold film and defect annihilation might be the main reason of the tensile stress increase in the present study.…”
Section: Residual Stress Increase After Thermal Holdingsupporting
confidence: 55%
“…In the limited regime (T < 125 C) [15,16], higher temperature can facilitate a series of thermally activated processes and would lead to a faster and more thorough recovery process. As the consequence, change of the residual stress due to recovery is much significant at higher temperature.…”
Section: Residual Stress Increase After Thermal Holdingmentioning
“…This is in Table 1 Experiment procedure of cyclic aging and annealing of gold films. 1 NP TH NP TH TH NP TH TH NP TH TH TH NP TH TH TH TH accordance with the literature that twins are seen frequently in gold thin films due to low stacking fault energy [16]. Ignoring the twin boundaries, an irregular column structure can be clearly seen.…”
Section: Resultssupporting
confidence: 87%
“…The same effect can also be used to explain the tensile stress generation during post-deposition annealing. Miller [14e16] indicated that defect annihilation was the reason for tensile stress generation caused by annealing in a limited regime (T < 125 C) [15,16]. The SEM and STEM micrographs revealed that an abundance of defects exist in the as deposited gold film and defect annihilation might be the main reason of the tensile stress increase in the present study.…”
Section: Residual Stress Increase After Thermal Holdingsupporting
confidence: 55%
“…In the limited regime (T < 125 C) [15,16], higher temperature can facilitate a series of thermally activated processes and would lead to a faster and more thorough recovery process. As the consequence, change of the residual stress due to recovery is much significant at higher temperature.…”
Section: Residual Stress Increase After Thermal Holdingmentioning
“…The modulus of 115.3 GPa and Poisson's ratio of 0.37 might be expected for the gold, based on the 〈111〉 anisotropic values, i.e., the dominant texture of the gold films. 25,[32][33][34] The indentation of a single crystal has been studied, even for the case of highly anisotropic material. 35,36 These studies suggest that the Hill material property values (the average of the isostress and isostrain conditions) are reasonable estimates, even when indenting anisotropic single crystals.…”
Section: Data Reduction Models and Methodsmentioning
confidence: 99%
“…After being cut to size, separate specimens were annealed at room temperature or 177°C for 4 h. The annealing temperatures are sufficiently low that the 20-nm-thick chromium layer, used to adhere the gold to the polycrystalline silicon underneath, was not observed to diffuse into the other materials. 25 A Nano DCM (MTS Systems Corp., Minneapolis, MN) was used to indent into the specimens with a diamond Berkovich tip at room temperature. When performed in "continuous stiffness" mode, 26 instrumented indentation can be used to obtain the hardness and modulus of a material at discrete instances (unloading events) throughout its thickness, according to the Oliver-Pharr method.…”
We studied the deformation mechanisms and mechanics during indentation of polycrystalline gold thin films at depths below 100 nm. The measured material hardness decreased from 2.1 ± 0.1 to 1.7 ± 0.1 GPa after annealing for 4 h at 177°C. Upon closer inspection, the hardness trends in the gold thin films were discovered to vary according to the indentation depth. At nanometer depths, the material hardness was quantified using multiple parameters, some of which were independent of the area calibration for the tip. The annealed specimen was very "hard" at low indentation depths, relatively soft at moderate indentation depths, and finally harder until the grain-size limit was reached. The as-deposited specimen demonstrated a relatively continuous harness trend as function of indentation depth, exhibiting monotonic convergence to Hall-Petch limited behavior. Discrete displacement jump events (excursions or "pop-ins") were frequently observed for the annealed specimen but not for the as-deposited specimen. Variation in hardness, excursion activity, and displacement during the hold at maximum load was observed according to the applied loading, which was parametrically varied at constant strain rates. Hardness results are explained in terms of the population and evolution of defects present within the specimens. The population of point defects is also influential, and critical thermal fluctuations, as well as the thermally activated process of diffusion, are believed to influence hardness at the specimen's free surface and further into its volume. After converging to a monotonic trend (proper tip engagement), the modulus of the gold was measured to be 106.0 ± 12.9 and 101.3 ± 6.0 GPa for the respective Au/Cr/Si specimens. These values exceeded predictions from the aggregate polycrystalline material theory, a representation used to estimate results for anisotropic single crystals. Exaggerated modulus measurements are explained as the result of the contribution of modulus mismatch with the substrate, pileup at the indentor tip, residual stress in the films, and crystallographic anisotropy of the gold.
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