3.1. Material Characterization
Figure 3 depicts the surface morphology of test specimens both before and after water vapor treatment. Consistent with previous findings for Zn-Mg-Al, lamellar structures are evident in the Zn-matrix phase, Zn-MgZn2 binary, and Zn-MgZn2-Al ternary phases, as indicated by the elements presented in the surface composition of the bare specimen in
Table 1. Specifically, examination of the bare specimen’s surface in
Figure 3(a) reveals the presence of the Zn-matrix phase and Zn-MgZn2-Al ternary phase [
12]. Following water vapor treatment,
Figure 3(b) illustrates the destruction of the lamellar structure, replaced by a diffusion-like shape. Region (3), distinguished by the highest O content and a rough surface, is presumed to have undergone the most substantial oxide formation during water vapor treatment. This suggests that the occurrence of light scattering due to surface roughness may contribute to blackening. Conversely, regions (1) and (2), retaining the lamellar structure and undergoing diffusion, exhibit comparatively less oxide formation, as indicated by the elements present in the surface composition of the Bare ST specimen in
Table 2. Analysis of the oxygen composition in Bare ST suggests that an increase in the ratio of oxygen elements is associated with the advancement of blackening.
Similarly to the surface morphology results observed in
Figure 3, when examining the cross-sectional morphology of the Bare specimen in
Figure 4, it was confirmed that a lamellar structure is formed between the intermetallic compounds. Additional TEM analysis with EDS mapping revealed predominantly formed Zn, and when confirming the point element composition in the region where Mg elements were mapped, it was determined to be 23.99 at% Mg and 71.75% Zn. This suggests the formation of the intermetallic compound MgZn2. Furthermore, Al was found to be distributed around Zn and Mg, similar to the results observed on the surface. Oxygen, as seen in the mapping, was found to be extremely thin near the surface, indicating the presence of a naturally formed oxide layer on the metal surface.
In contrast,
Figure 5 shows the examination of cross-sectional morphology and EDS mapping of Bare ST, where it was observed that the lamellar structure, akin to the surface morphology, was disrupted and appeared to be diffusing. This phenomenon was attributed to surface treatment occurring due to high-temperature steam. Through EDS mapping to confirm the shapes of each element, it was evident that the boundaries were clearly defined in Bare, while in Bare ST, all elements were diffused. Particularly, oxygen (O) was found to be formed approximately 5 μm deep from the surface. This led to the conclusion that an oxide layer formed through steam treatment on the surface.
Figure 6 presents the depth-wise elemental composition analysis results from the surface analyzed through GD-OES. When examining the depth-wise elemental composition of Bare, it was observed that Zn predominantly occupied the surface, consistent with the composition of the test specimen. Small amounts of Mg and Al were also detected, and Fe showed an increase from a depth of 10 μm, intersecting with the decreasing Zn, indicating the formation of an approximately 10 μm alloy coating on the specimen.
Unlike Bare, in the case of Bare ST, a higher proportion of O was observed on the surface, with the proportion gradually decreasing to a depth of about 5 μm. Additionally, the depth of the coating layer was approximately 14 μm, with a surface oxide layer of 5 μm thickness. This observation indicates an increase in the thickness of the oxide layer. This observation aligns with the results obtained through TEM’s oxygen mapping, supporting the hypothesis that the main factor contributing to blackening is the formation of an oxide layer on the surface.
Next, we analyzed the crystal structure and phase information of the test specimen film using XRD. As seen in
Figure 7, peaks for mostly Zn and MgZn2 are detected in the Bare specimen. In contrast, after the water vapor treatment, Bare ST specimen’s peaks for oxides such as zinc oxide (ZnO) and hydrated oxides such as Mg(OH)
2 were detected. It was judged that oxides were formed on the surface, similar to the EDS composition analysis, and it was confirmed that hydrated oxides were also formed on the surface. Based on the ZnO peak from the XRD analysis, the crystal size and interplanar spacing were analyzed using Bragg’s law in equations 1 and 2. It was found that the interplanar spacing of ZnO increased after the water vapor treatment through
Figure 8 [
13]. This is presumed to result from a chemical state change or oxygen vacancy, as illustrated in
Figure 9 [
14].
In addition, the crystal structure was verified through XPS spectra analysis, as illustrated in
Figure 10 and
Figure 11. Following water vapor treatment, discernible peaks emerged in the binding energy of the oxide and hydroxide in the Zn 2p, Mg 1s, and Al 2p results, corroborating the formation of oxide and hydroxide, in line with the findings from XRD.
Upon scrutinizing the Zn LMM spectra for the oxygen Auger peak in the Bare specimen, a peak indicative of Zn
2+ ion binding was observed. Conversely, in the Bare ST specimen post-steam treatment, a peak corresponding to Zn
1+ binding was identified. This observation suggests a shift in the ZnO peak after steam treatment, signifying a transformation from ZnO to ZnO
1-x. The alteration is likely attributed to the change in oxidation state during the transformation from ZnO to ZnO
1-x. Furthermore, as depicted in
Figure 11, the O1s binding energy peak was subjected to fitting, revealing three distinct peaks with binding energies of approximately 530.2, 530, and 528 eV, respectively. The lowest binding energy is associated with the metal-oxygen bond (M-O), such as ZnO or MgO, the intermediate energy corresponds to oxygen vacancy, and the highest energy is linked to the bond with moisture on the metal surface (OH
-) [
15]. Notably, oxygen vacancy was not detected in the sample before water vapor treatment, but its occurrence was confirmed after treatment. Consequently, the observed increase in the interplanar distance of ZnO, as evidenced in the XRD results, is attributed to the occurrence of oxygen vacancy in ZnO, leading to the formation of an oxygen-deficient oxide
(2) Optical Characterization
Figure 12 illustrates the analysis of optical properties using UV-Vis-nir to measure reflectance across the wavelength range of 0-2500 nm. Upon measuring reflectance, it was observed that the black specimen exhibited low reflectance, akin to the brightness depicted in
Figure 2. For the conversion of reflectance to absorbance, representing the extent of light absorption, the Kubelka-Munk equation (equation 3) was applied [
16]. Upon examining the absorbance results, a sharp increase was observed around 390 nm in the visible light range for the black specimen after water vapor treatment, suggesting absorption of visible light by a certain factor, as depicted in
Figure 12.
This is attributed to the absorption of visible light resulting from ZnO defects caused by an increase in interfacial distance due to oxygen vacancies, as revealed in the preceding XRD and XPS analyses. In addition, the band gap was measured based on the obtained absorbance using the Tauc plot. The Tauc plot graph can be obtained by using photon energy and optical energy as the x and y axes, respectively, and the formulas for obtaining photon energy and optical energy are shown in Equation 4 and Equation 5 [
17].
Derived from the absorbance, the band gap of Bare ST was calculated to be approximately 2.92 eV, as illustrated in
Figure 13. This value is lower than the typical band gap of ZnO, which is 3.4 eV, indicating that the band gap energy decreases with the proportion of oxygen in ZnO [
18]. Hence, the band gap measurement implies the presence of oxygen deficiency in ZnO. As observed in
Figure 14., the reactive Mg and Al ions combine with oxygen to form ZnO
1-x, an oxygen-deficient oxide, by extracting oxygen from ZnO.