Similarly to Figure 4, the plots present values averaged from sev

Similarly to Figure 4, the plots present values averaged from several measurements made on three different samples evaporated at each temperature. Surprisingly, in 10-nm-thick films in the whole range of temperatures 200 to 350 K, adhesive forces between Ag adatoms and Ge wetting layer dominate over cohesive forces in silver. Thus, the temperature-dependent mobility of Ag adatoms does not deteriorate significantly the surface smoothness. RMS roughness values from tapping-mode AFM measurements of 10-nm Ag films are in agreement with those obtained using

XRR. An example of XRR data obtained for the 10-nm-thick Ag film deposited on 1-nm Ge interlayer and a fitted model are shown in Figure 7. The average film thickness measured HDAC inhibitor using XRR is 10.9 ± 1.1 nm and differs up to 10% from the buy C188-9 values controlled with calibrated quartz weight installed in the vicinity of substrates in the vacuum chamber of the e-beam evaporator. In single-layer structures, e.g., plasmonic silver lenses [28, 29], such fabrication

inaccuracies should less deteriorate performance than in the case of metal-dielectric-layered flat lenses [30–32]. Figure 6 Ten-point and average height values measured on 3 × 3 μm 2 area on 10-nm Ag films. Thin films were deposited at temperatures in the range 200 to 350 K, and RMS values were measured using both AFM and XRR. Figure 7 XRR data and fitted model for 10-nm Ag and 1-nm Ge film on sapphire substrate. At the end, we investigated the interior structure of 10-nm-thick samples using one-dimensional XRD. The dependency between grain size and the substrate temperature is presented in Figure 8. Again, the samples evaporated at temperatures close to RT have the best uniformity. Figure 8 Grain sizes measured using one-dimensional XRD. Ag films of 10-nm thickness were deposited at temperatures in the range 200 to 350 K. Conclusions A new sublimation-pressure empirical equation valid in the range from 50 K to T t = 273.16 K of the triple point helps Urocanase https://www.selleckchem.com/products/q-vd-oph.html select the optimum temperature in high-vacuum physical vapor deposition systems. We have demonstrated the possibility

to fabricate ultrasmooth metal nanolayers deposited onto epi-polished substrates at the lowest achievable pressure and at such a temperature that the whole dynamic range of both parameters is located on the gas side of the phase-boundary curve of water in a p-T diagram. The temperature range 230 to 350 K is established as the optimum for deposition of Ag nanolayers using e-beam evaporators. For the 10-nm Ag film on 1-nm Ge interlayer deposited at RT on sapphire substrate, a surface roughness with RMS = 0.22 nm has been achieved. For 30-nm-thick Ag films on sapphire substrate with 1-nm Ge wetting layer, RMS increases up to 0.49 nm. The ten-point height parameter given by extreme local surface features, which reflects scattering properties, has its minimum at 295 K.

Comments are closed.