The obtained selleck kinase inhibitor values strongly indicate that we deal with a compressive stress exerted on the Si-NCs which shifts the observed Raman lines towards higher wavenumbers [4]. Similar effect has been observed for Si-NCs obtained by chemical vapor deposition technique and annealed at 1,250°C [19]. Moreover, the observed rise of ω c indicates that the stress increases as a function of r H. Assuming that the hydrostatic pressure of about 1 GPa results in approximately 1.88 cm−1 shift
of the Raman line [20], we may estimate the maximum this website stress to be about 2.6 GPa for r H = 50% sample. The obtained results also explain why we do not observe a clear downshift of the Raman frequency related to PC effect. Namely, the compressive stress increases as a function of r H and compensates for the downshift due to the finite crystallite size. It is worth to note that PC effect has been actually observed for Si-NCs synthesized in the form of free-standing powder [21]. Therefore, the difficulties
related to the observation of this effect in our case seem to be matrix-related. It should be also noted here that the obtained values of ω c do not strongly depend on the PC model selection. To check this, we fitted the HF Raman band with another PC model proposed by Campbell et al. [15] (with a Gaussian weighting function instead of sinc). Although this model predicted overestimated Si-NCs sizes (4 nm for r H = 50% and 5 nm for r H = 10%), the obtained values of ω c were similar (ω c = 523 cm−1 for r H = 10% and ω c = 524 cm−1 for r H = 50%). It should also be mentioned that both models are simplified since they do not take into account find more such effects as stress distribution or Si-NCs size distribution. Therefore, the estimated stress values should be treated as estimation. In the next step, the Raman results were used to calculate the relative contribution of the HF (Si-NCs) and LF (a-Si) bands to the total Raman scattering, according to the following equations: (5) where the intensities I Si-NC and I A are defined
as Fenbendazole integrals over ω of Equations 1 and 3, respectively. We prefer to calculate the relative contributions instead of the absolute amorphous and crystalline fractions since, as shown by Ossadnik et al. [22], the Raman-based estimates of the latter can be very inaccurate. Figure 2a shows the relative contributions of the HF (Si-NCs) and LF (a-Si) bands to the total Raman scattering intensity as a function of r H. It can be seen that the relative contribution from Si-NCs drops with r H, which we believe reflects a relative drop of the crystalline fraction. Simultaneously, we observe a relative increase of the amorphous fraction with r H. These results are in agreement with our previous structural investigations for similar structures, where it has been shown that increase of r H results in the increase of the amount of a-Si in the structures.