465). This leads to the formation of small mound-like entities (in the form of broken ripples) appearing on the corrugated surface. For further investigation on the role of shadowing effect in morphological evolution, we extracted line profiles of the observed structures along the Protein Tyrosine Kinase inhibitor direction of incident ion beam onto the surface as shown by the arrow marks on the respective AFM images. Line profiles obtained from Figures 3b,c and 4a,b are shown in Figures 5 and 6, respectively. It is observed from Figures 5b and 6b that at the beginning of shadowing transition, the line profiles are still sinusoidal in nature. As discussed previously,

beyond shadowing transition, one would expect signature of sawtooth-like waveform. The fact that Nec-1s cell line for both incidence angles sawtooth-like waveform is not yet formed www.selleckchem.com/products/MGCD0103(Mocetinostat).html may be attributed to early stage of shadowing where h 0/λ ratios are very close to the limiting values or little above. To check this, line profiles obtained from Figures 3d and 4c (corresponding to a higher fluence of 5 × 1017 ions cm-2) are shown in Figures 5c and 6c which clearly show a transition to sawtooth-like waveform. This is due to the fact that h 0/λ ratios (in both cases) are well beyond the respective shadowing limits (0.767 and 0.741, respectively).

Thus, we can infer that the effect of ion beam shadowing plays a dominant role in the transition from rippled surfaces to faceted structures and is expectedly more prominent for the higher incidence angle as is evident from the previous discussion. Figure 5 Line profiles extracted from the AFM images of ion-exposed samples at 70°. Various fluences: (a) 1 × 1017, (b) 2 × 1017, (c) 5 × 1017, (d) 10 × 1017, (e) 15 × 1017, and (f) 20 × 1017 ions cm-2, respectively. Arrow indicates the direction of ion beam onto the surface. Figure 6 Line profiles extracted from the AFM images of ion-exposed samples at 72.5°. Different

ion fluences: (a) 1 × 1017, (b) 2 × 1017, (c) 5 × 1017, (d) 10 × 1017, (e) 15 × 1017, and (f) 20 × 1017 ions cm-2, respectively. Arrow indicates the Molecular motor direction of ion beam onto the surface. We now go on to explain the coarsening behaviour of faceted structures (as is evident from Table 1) at higher fluences (>5 × 1017 ions cm-2) using the mechanism proposed by Hauffe [32]. In this framework, the intensity of reflected ions impinging on an arbitrary area on a facet depends on the dimensions of the reflecting adjoining facets. According to V n ~ jY, where j is the ion density on the surface element (which also contains the reflected ions), Y is the sputtering yield, and V n is the displacement velocity of a surface element in the direction of its normal, it is clear that the displacement velocity will be higher for the larger facet. This does not require a particular form of spatial distribution of reflected ions albeit it is necessary that the reflected ions should fall on the neighbouring facets.