have gained a lot of interest. The iridates indeed display SOC which is on a similar energy scale than that of the electroncorrelation or the electronic bandwidth, [1] which favors new or exotic quantum electronic states. [2][3][4][5][6] However, in contrast to archetypical correlated 3d TMOs, the electron-electron correlation strength is often too small in the 5d TMOs to host ferromagnetism.For Sr 2 IrO 4 (n = 1), the SOC results in a spin-orbital mixed state of the Ir 4+ ion with a filled quadruplet pseudospin state J eff = 3/2 and a half-filled doublet J eff = 1/2. [7] Magnetic interaction of neighbored pseudospins leads to a basal (ab)-plane canted antiferromagnetic (AFM) Mottinsulator ground state with pseudospins locked to the oxygen octahedral rotation. [8][9][10] For n = 2, interlayer coupling weakens which leads to a spin-flop transition of the pseudospins with out-of-plane spin alignment along the c-axis and T N = 280 K. [11] In contrast, the perovskite phase SrIrO 3 (SIO) (n = ∞) displays paramagnetic semimetallic behavior due to an increased hybridization of Ir5d and O2p orbitals. [3,[12][13][14][15] Nevertheless, SIO is on the verge of a magnetic ground state and may display AFM or ferromagnetic (FM) properties as well, depending on the details of the Hubbard interaction U and the SOC. [12] Owing to a strong pseudospin-lattice coupling, [16] these can be finely tuned by structural modifications, especially with respect to the network of the corner-sharing IrO 6 octahedra which in turn enables a manipulation of the magnetism in SIO.The bulk structure of SIO consists in a distorted orthorhombic perovskite structure with in-phase and antiphase rotations of the IrO 6 octahedra (a − a − c + in Glazer notation). [17,18] However, a suppression of octahedral out-of-plane tilts, akin to the rotation pattern of Sr 2 IrO 4 can be achieved when ultrathin SIO films are epitaxially grown on cubic SrTiO 3 (STO) which concomitantly yields a metal-to-insulator transition (MIT). [19] Other type of structural distortions are likewise discussed as a possible source for magnetic properties of SIO. [20] For example, in SIO/STO superlattices the IrO 6 rotation pattern supports an AFM ground state, [21,22] where the ordering temperature T N can be controlled by the interlayer coupling, i.e., by the STO thickness [23] or epitaxial strain. [24] Meanwhile a lot of activities have been focused on SIO-based heterostructures including magnetic active layers, which seems The 5d iridium-based transition metal oxides have gained broad interest because of their strong spin-orbit coupling, which favors new or exotic quantum electronic states. On the other hand, they rarely exhibit more mainstream orders like ferromagnetism due to generally weak electron-electron correlation strength. Here, a proximity-induced ferromagnetic (FM) state with T C ≈ 100 K and strong magnetocrystalline anisotropy is shown in a SrIrO 3 (SIO) heterostructure via interfacial charge transfer by using a ferromagnetic insulator in contact with SIO. Electrical tra...