Rutile‐ and anatase‐type temperature‐dependent pre‐edge peak intensities in K ‐edge XANES spectra for A O ( A = Mn), A 2 O 3 ( A = Sc, Cr and Mn) and A O 2 ( A = Ti and V)

Pre‐edge peaks in 3 d transition‐metal element (Sc, Ti, V, Cr and Mn) K ‐edge XANES (X‐ray absorption near‐edge structure) spectra in A O 2 ( A  = Ti and V), A 2 O 3 ( A  = Sc, Cr and Mn) and A O ( A  = Mn) are measured at various temperatures. Quantitative comparisons for the XANES spectra were investigated by using absorption intensity invariant point normalization. The energy position of the difference peak (D peak) is obtained from the difference between the low‐ and high‐temperature XANES spectra. There are two kinds of temperature dependence for pre‐edge peak intensity: rutile‐ and anatase‐type. The true temperature dependence of a transition to each orbital is obtained from the difference spectrum. In both anatase and rutile, the pre‐edge peak positions of A2 and A3 are clearly different from the D1‐ and D2‐peak positions. The A1 peak‐top energies in both phases of VO 2 differ from the D1 peak‐top energies. The D‐peak energy position determined by the difference spectrum should represent one of the true energies for the transition to an independent orbital. The peak‐top positions for pre‐edge peaks in XANES do not always represent the true energy for independent transitions to orbitals because several orbital transitions overlap with similar energies. This work suggests that deformation vibration (bending mode) is effective in determining the temperature dependence for the D‐peak intensity.