Several materials properties of rutile TiO 2 (together with its other polymorphs) have been widely investigated in view of both fundamental and practical interest. It is a wide band gap (E g ¼ 3.05 eV) semiconductor that finds application, among others, as a photocatalyst for splitting water [1] into H 2 and O 2 and remediation of organic pollutants. [2] Among the lesswell-known properties of TiO 2 is its abnormally large static dielectric permittivity that shows strong frequency dependence as well as the associated soft A 2u mode that decreases with decreasing temperature. [3,4] The latter, however, never becomes completely soft, even at 0 K. Accordingly, rutile is classified as an incipient ferroelectric. We prepared M 0 TiTaO 6 (M 0 ¼ Al, Cr, Fe) oxides by conventional solid-state synthesis starting from pure binary oxides. Powder X-ray diffraction (XRD) showed formation of rutile structure for all three M 0 TiTaO 6 compounds. All the reflections in the patterns (Fig. 1) could be indexed to the tetragonal rutile structure. The structural parameters derived from Rietveld refinement of the powder XRD data are given in Table 1. We see that while the c/a ratio remains nearly the same as in the parent rutile TiO 2 , the a and c parameters of M 0 TiTaO 6 show variations that are consistent with the average ionic radii of the metal atoms. We find that the average M-O distances in FeTiTaO 6 are slightly larger than those in rutile, consisting of 4 short and 2 long M-O bonds (elongated MO 6 octahedron); curiously, for M 0 ¼ Al and Cr oxides we find 4 long and 2 short M-O bonds (compressed MO 6 octahedron).We have recorded neutron diffraction (ND) patterns of M 0 ¼ Cr, Fe at T ¼ 300, 150, and 12 K, in an attempt to characterize further the structure of these oxides. We see no evidence for a long-range magnetic ordering down to 12 K in