“…The diffraction peaks of Yb 2 O 3 were determined at 2θ = 20.5, 29.3, 34.1, 44.06, 49.1, 53.9, and 58.4°, which correspond to Miller’s indices (211), (222), (400), (622), (440), (611), and (622) [ 19 ]. The high, intense peak was at 29.3; however, peaks at 49.1 and 58.4° were ascribed as weak diffraction peaks that refer to the cubic structure of Yb 2 O 3 [ 20 ]. In addition, V 2 O 5 exhibited several peaks at 2 θ = 15.08, 20.6, 26.03, and 30.7°, which correspond to the orthorhombic structure of V 2 O 5 with Miller’s indices (200), (001), (110), and (301) [ 21 ].…”