2018
DOI: 10.1007/s10854-018-0406-1
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Optical properties of p-type SnOx thin films deposited by DC reactive sputtering

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Cited by 16 publications
(11 citation statements)
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“…In the as-deposited state (upper), the HR O 1s spectrum exhibits slight asymmetry in the peak that is deconvoluted into two peaks, one at 529.64 eV (strong) due to lattice oxygens in SnO x and another at 530.67 eV (weak) attributed to the presence of oxygen-related defects or the hydroxyl group. 67 After annealing (lower), the overall peak location shifted toward higher binding energy by approximately 0.94 eV, which results from the crystallization reaction during annealing, leading to a higher binding energy of oxygen in the annealed SnO x . It should also be noted that no significant asymmetry is observed in the annealed HR O 1s spectrum, which can be understood by the fact that the oxygen defects present in the as-deposited state were oxidized during annealing in air.…”
Section: Resultsmentioning
confidence: 99%
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“…In the as-deposited state (upper), the HR O 1s spectrum exhibits slight asymmetry in the peak that is deconvoluted into two peaks, one at 529.64 eV (strong) due to lattice oxygens in SnO x and another at 530.67 eV (weak) attributed to the presence of oxygen-related defects or the hydroxyl group. 67 After annealing (lower), the overall peak location shifted toward higher binding energy by approximately 0.94 eV, which results from the crystallization reaction during annealing, leading to a higher binding energy of oxygen in the annealed SnO x . It should also be noted that no significant asymmetry is observed in the annealed HR O 1s spectrum, which can be understood by the fact that the oxygen defects present in the as-deposited state were oxidized during annealing in air.…”
Section: Resultsmentioning
confidence: 99%
“…Core-level HR O 1s XPS spectra are shown in Figure b. In the as-deposited state (upper), the HR O 1s spectrum exhibits slight asymmetry in the peak that is deconvoluted into two peaks, one at 529.64 eV (strong) due to lattice oxygens in SnO x and another at 530.67 eV (weak) attributed to the presence of oxygen-related defects or the hydroxyl group . After annealing (lower), the overall peak location shifted toward higher binding energy by approximately 0.94 eV, which results from the crystallization reaction during annealing, leading to a higher binding energy of oxygen in the annealed SnO x .…”
Section: Results and Discussionmentioning
confidence: 99%
“…A typical X-ray diffractogram shown in Figure 1(b) exhibits a (Figure 1e) was also determined to be ∼0.88 eV from a Tauc plot for the indirect transition of (α) 1/2 vs hν, which is matched with the values (∼0.7−1.0 eV) found from previous studies, of which the indirect E g values were estimated from absorption spectra and theoretical calculations. 8,47,52,53 Cross-sectional microstructures and elemental distributions were investigated through TEM and EDS. annular dark-field (HAADF) TEM image (Figure 1g) and its associated EDS elemental mapping (Figure 1h,i) were obtained from a SiO 2 /p-SnO x sample.…”
Section: Resultsmentioning
confidence: 99%
“…The bandgap was a little different for the SnO x thin film deposited at a ppO 2 of 18.5% (2.86 eV), although the rest of the n‐type samples showed a bandgap in the range obtained for the p‐type samples. Noteworthy, those bandgap values are indicative of high transparency in the p‐ and n‐type SnO x thin films, which allows the fabrication of p–n homo‐junctions using transparent SnO x thin films 35 …”
Section: Resultsmentioning
confidence: 99%