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It is rather hard to discern the (Equation presented) peak in the He II spectrum due to its overlapping with a stronger satellite feature generated by unmonochromated He II radiation [Fig. 3(b)]
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It is rather hard to discern the (Equation presented) peak in the He II spectrum due to its overlapping with a stronger satellite feature generated by unmonochromated He II radiation [Fig. 3(b)].
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84940067222
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The apparent shift of the (Equation presented) and (Equation presented) peaks toward a higher binding energy in Figs. 3(c) and 3(d) is due to band bending that gradually increases upon further hydroxylation and reduction (Fig. S4)
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The apparent shift of the (Equation presented) and (Equation presented) peaks toward a higher binding energy in Figs. 3(c) and 3(d) is due to band bending that gradually increases upon further hydroxylation and reduction (Fig. S4).
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The width of the (Equation presented) peak also proportionally increases with (Equation presented) coverage (Fig. S5), which is consistent with a growing electron population of the band-gap defect state upon further reduction
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The width of the (Equation presented) peak also proportionally increases with (Equation presented) coverage (Fig. S5), which is consistent with a growing electron population of the band-gap defect state upon further reduction.
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