The race to obtain a higher critical temperature (T c ) in the superconducting cuprates has been virtually suspended since it was optimized under high pressure in a hole-doped trilayer cuprate. We report the anomalous increase in T c under high pressure for the electron-doped infinite-layer cuprate Sr 0.9 La 0.1 CuO 2 in the vicinity of the antiferromagnetic critical point. By the application of a pressure of 15 GPa, T c increases to 45 K, which is the highest temperature among the electron-doped cuprates and ensures unconventional superconductivity. We describe the electronic phase diagram of Sr 1−x La x CuO 2 to discuss the relation between the antiferromagnetic order and superconductivity.KEYWORDS: high-T c cuprates, electron-doped cuprates, high pressure, infinite-layered structure Electron-hole symmetry/asymmetry has been conceived as one of the most important features of the high-T c cuprates. 1-3) The asymmetry is manifested in generic phase diagrams as a function of the doping level. The antiferromagnetic (AF) phase exists in a low and narrow doping range for the hole-doped cuprates, whereas that for the electron-doped cuprates remains up to a high doping level, allowing the emergence of superconductivity. However, the electronic phase diagram for the electron-doped cuprates relies only on results for the family of R 2-x Ce x CuO 4 (R: rare-earth metal) 4,5) , which leaves uncertainty in discussions on the generic electron-hole asymmetry. For an other electron-doped cuprate, infinite-layer Sr 1-x R x CuO 2 with the optimum T c of 43 K, while the superconductivity has been investigated as a function of x, [6][7][8][9] the relation between the AF order and the superconductivity remains unclear. Since Sr 1-x La x CuO 2 contains no magnetic cations other than the Cu ion, the interplay