Structural studies of the ferrimagnetic (T N =200 K) Mott insulator GaFeO 3 (SG Pc2 1 n) to 70 GPa, complemented by 57 Fe Mössbauer spectroscopy and resistance (R) measurements at compression, decompression and recompression reveal a fascinating sequence of structures. Starting at ~ 25 GPa a new structure, an orthorhombic perovskite (SG Pbnm), is sluggishly formed followed by a volume V(P) drop of 5.4%. The complete formation of the perovskite occurs at 42 GPa. In the 0 -33 GPa range T N reaches 300 K and R(P) decreases by one-order of magnitude. At 53 GPa an isostructural transition is detected, characterized by a discontinuous drop of V(P) by ~3%. Mössbauer spectra reveal a non-magnetic component coexisting with the magnetic one at ~ 60 GPa. Its abundance increases and above 77 GPa no sign of a magnetic hyperfine interaction is detected down to 5 K.Concurrently, one observes a continuous yet precipitous decrease in R(P) taking place in the 53-68 GPa range, leading to an onset of the metallic state at P = 68 GPa. These electronic/magnetic features of the high pressure (HP) perovskite are consistent with a Mott transition.With pressure decrease, below 50 GPa, the insulating perovskite is recovered, and at ~24 GPa a 1 storder structural transition takes place to a LiNbO 3 -type structure with SG R3c. This structure remains stable down to ambient pressure and with recompression it is stable up to 50 GPa, afterwards it transforms back to the HP perovskite structure. It is noteworthy that this transition occurs at the same