HIGH-TEMPERATURE INTERGROWTH STRUCTURES IN Fe2Oa-TiO2viewed along [012] r. It is seen that it comprises two interpenetrating sets of (111) strings of edge-linked octahedral face-shared dimers, the directions of both strings being different from that in the low-temperature (121)r precursor phase, Fig. 14(a). In transforming_ to the high-temperature phases, the integrity of the [111 ]r strings is lost, but the l l0i], strings of corner-linked face-shared octahedral pairs persist.A high-resolution electron-imaging and diffraction study of the transformation mechanism has been carried out and will be reported elsewhere (Bursill & Grey, 1977). This study shows (121)~ and (i2i) r CS structures intersecting to form (101)~ interfaces containing the [10i]r strings common to both high-and low-temperature structures. These [10i]~ structural features (imaged edge-on in Figs. 3 and 4) provide the key to the structural relations and the reaction mechanism. It is interesting to note that the hightemperature structures may be derived mathematically as follows:
I (020)r= (121)r + (i2i).II (Okl)r=P(020) r + q(011) r.The element (011)r represents the same anti-phase component required for swinging in the lowtemperature structures.