-4 Pa and then in air at T = 800 0 C leads to the destruction of its initial grain structure and to its chemical separation into two phases: (i) oxygen stoichiometric A-site ordered PrBaMn 2 O 6 with tetragonal (SG = P4/mmm, Z = 2) unit cell and T C ≈ 313 K and (ii) oxygen superstoichiometric A-site disordered Pr 0.90 Ba 0.10 MnO 3.05 with orthorhombic (SG = Pnma, Z = 4) unit cell and T C ≈ 133 K. It also exhibits a magnetoresistance of ~ 14 % at ~ 313 K in a field of 50 kOe. This processed sample has a reduced average grain size 〈 D 〉 ≈ 491 nm. The observed magnetic properties are interpreted in terms of chemical phase separation, grain size, and A-site ionic ordering effects. The materials obtained in this work may be used at the creation of the magnetic field sensors, as they have considerable magnetoresistance ( ~14% in field of 50 kOe) at room temperature.