3.1. X‑Ray Diffraction Technique
X-ray diffraction (XRD) is a valuable technique for studying the structure of polymeric materials, providing insights into parameters such as crystallite size, degree of crystallinity, dislocation density, and microstrain. In this study, XRD analysis was conducted to investigate the influence of ZnO nanoparticles on the structure of the PS polymer matrix. Figure 1 presents the diffraction pattern of pristine PS and PS/ZnO nanocomposites. The spectrum exhibits a broad peak around 2θ value of 20°, indicating the amorphous nature of the PS film [25, 26].
A broad suppressed peak at 20° is observed for pristine PS, which diminishes as ZnO is introduced into the PS matrix. With increasing ZnO content from 1 to 10 wt%, new sharp and intense peaks emerge at 31.71°, 34.53°, 36.26°, 48°, 56.67°, 62.85°, 66°, and 68.07°, as depicted in the spectra of the nanocomposite films. These peaks correspond to the presence of ZnO within the PS polymer matrix, aligned with the Miller indices (100), (002), (101), (102), (110), (103), (200), (112), and (201), respectively. They become more prominent with increasing ZnO wt%. Comparison of these peaks with the XRD peaks of ZnO nanopowder and JCPDS file confirms the presence of ZnO.
The average crystallite size (D) for the nanocomposites was estimated using Scherrer’s formula, where D represents the grain size (or crystalline size) of the material, λ is the wavelength of the X-ray beam, θ is the diffraction angle, β is the full width at half maximum (FWHM) of the observed peak in radians, and K is a constant called the shape factor, equal to 0.89 [27, 28, 29, 30]. The average grain sizes (or crystalline sizes) were found to be 3.88 nm, 3.41 nm, and 1.58 nm, respectively, for the polystyrene/1% ZnO NC, polystyrene/5% ZnO NC, and polystyrene/10% ZnO NC. The addition of ZnO resulted in a gradual increase in crystalline size due to its large surface area.
3.2. UV–VIS Spectroscopy
The effect of zinc oxide nanoparticles on optical absorbance of PS was studied through UV-vis spectra. UV–Visible spectra of nanocomposite films was recorded in the wavelength range of 250–600 nm. Figure 1 illustrates the absorption spectra of pristine PS and PS/ZnO nanocomposite films. The presence of ZnO induces an absorption band at 370 nm, consistent with findings from previous studies [31, 32]. As the filler content increased, this peak expanded and moved to a longer wavelength (red-shifted). This change clearly shows that nanoparticles agglomerate as their content increases. The spectra reveal that the absorbance of the polymer increases with rising concentrations of ZnO nanoparticles, likely attributed to the increased number of charge carriers within the nanocomposite [33].
The absorption coefficient (αhν)2 versus the wavelength (nm) for PS/ZnO nanocomposites is shown in Figure 3.
For a clear comparison, the calculated Eg values for the investigated PS/ZnO nanocomposites are listed in Table 1.
Table 1. Pure polystyrene (PS) and PS/ZnO based nanocomposites band gap (Eg)
Samples
|
Eg (Calculated using conventional extrapolation of Tauc’s plot) (eV)
|
PS
|
2,3 eV (539 nm)
|
PS/3%ZnO
|
3,2 eV (387 nm)
|
PS/5% ZnO
|
3,15 eV (393nm)
|
PS/10% ZnO
|
3,14 eV (391 nm)
|
The table shows that as the concentration of nanoparticles grew, the band gap Eg of the nanocomposites decreases (i.e., red-shifted), which is caused by the growing particle size. [34] In other words, as the nanoparticle content in the matrix increases, nanoparticle agglomeration occurs, leading to the formation of larger clusters and consequently a decrease in the optical band gap. The band gap reduction is consistent with the findings from PL investigations.
3.3. Photoluminescence (PL) Spectroscopy
Photoluminescence (PL) is a significant property that provides insights into the optically active defects and relaxation pathways for excited states. This study is essential for identifying the source of sub-band-gap luminescence. Figure 5 illustrates the photoluminescence (PL) spectra of PS/ZnO-based nanocomposites, depending on the volume content of ZnO nanoparticles. The presence of wide emission bands in the violet and blue regions suggests transitions from excitonic levels and/or zinc interstitials (Zni) to the conduction band, as well as contributions from defects such as zinc interstitials (Zni) and natural zinc vacancies (Znv) [36,37]. It is suggested that the origin of the violet emission at λ ~420 nm (2.95 eV) is due to the transitions from conduction band (CB) to the holes localized at defect level associated with zinc vacancy (V Zn ) [38]. The blue luminescence bands situated in (430–480) nm (2.8–2.68 eV) domain are due to transitions from extended donor Zni states and the holes in the valence band [38]. The blue-green emissions [480–510 nm] may be due to the transition from the oxygen inertial (Oi) and zinc antisites (OZn) to the valence band [39].
As can be seen from the PL spectra, the luminescence intensity increases depending on the concentration. At a certain volume content of the filler, it stops increasing and saturation occurs. This tendency is due to the increase in the size of the luminescent centers. The decrease in the luminescence intensity at a high amount of filler is explained by the fact that as the nanoparticle content increases, the probability of their agglomeration increases, which in turn significantly reduces the number of crystallization centers.