Space group assignment for a Perovskite compound is a complex task when only powder X-ray diffraction data obtained with K α (both K α1 and K α2 ) radiation is available. Whole profile refinement of powder X-ray diffraction data using Rietveld method is very good to check if the structural model is We reply to the preceding correspondence "Does BaTbO 3 Adopt the P1 Symmetry?" in this issue, [1] in which the authors challenge the crystal structure of BaTbO 3-δ that has been redetermined by us and published in this journal. [2] Several points need more discussion.The first point is the statement [1] that "… the space group P1 belongs to none of the space groups derived from the octahedral tilting". However, in the papers [3][4][5] cited in the correspondence by Fu and IJdo, [1] the space group P1 was indicated to be one of the space groups derived from the octahedral tilting. The space group P1 is strongly related to P1. The only difference is that P1 has a center of symmetry but P1 has not. All the space groups derived from the octahedral tilting [Pm3m (#221), P4/mbm (#127), I4/mmm (#139), Im3 (#204), Immm (71), I4/mcm (#140), Imma (#74), R3c (#167), C2/m (#12), C2/c (#15), P1 (#2), Cmcm (#63), Pnma (#62), P2 1 /m (#11), P4 2 /nmc (#137)], [5] have a center of symmetry. That means the tilting system always has a center of symmetry. It is also well known that BaTiO 3 and PbTiO 3 are perovskites without a center of symmetry at room temperature. [6] The tilting system thus does not cover all perovskites. As summarized by C. J. Howard and H. T. Stokes, [5] "Consequently, the majority of perovskites are in fact distorted perovskites (hettotypes). Three different types of distortions have been identified: distortions of the BX 6 octahedral units, B-cation displacements within the octahedra, and the tilting of the BX 6 octahedra relative to one another as practically rigid [a]