, Ti 2p (c), P 2p (d) and O 1s (e) for all LCGTP glass-ceramics under study. Spectrum line of C1s (f) for the C-C component resulting from adventitious carbon is also shown as a control. Note that intensities on the y-axis have been normalized to emphasize signal shapes rather than absolute intensities. Dashed lines represent BE peaks of LAGTP, Figure 5.30 -High-resolution XPS spectra of Cr 2p (a)
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