The outstanding optoelectronics and photovoltaic properties of metal halide perovskites, including high carrier motilities, low carrier recombination rates, and the tunable spectral absorption range are attributed to the unique electronic properties of these materials. While DFT provides reliable structures and stabilities of perovskites, it performs poorly in electronic structure prediction. The relativistic GW approximation has been demonstrated to be able to capture electronic structure accurately, but at an extremely high computational cost. Here we report efficient and accurate band gap calculations of halide metal perovskites by using the approximate quasiparticle DFT-1/2 method. Using AMX 3 (A = CH 3 NH 3 , CH 2 NHCH 2 , Cs; M = Pb, Sn, X = I, Br, Cl) as demonstration, the influence of the crystal structure (cubic, tetragonal or orthorhombic), variation of ions (different A, M and X) and relativistic effects on the electronic structure are systematically studied and compared with experimental results. Our results show that the DFT-1/2 method yields accurate band gaps with the precision of the GW method with no more computational cost than standard DFT. This opens the possibility of accurate electronic structure prediction of sophisticated halide perovskite structures and new materials design for lead-free materials.Hybrid organic-inorganic lead halide perovskites have become the jewel in the crown in the field of photovoltaics since the pioneering work by Kojima et al. and Im et al. 1,2 . In just four years the power conversion efficiency of solar cells based on hybrid perovskites has rapidly increased from an initial promising value of 9% 3 to over 22% 4 . In addition to the outstanding performance, simple and cost-effective fabrication, i.e. solution-processing techniques, render them one of the most desirable and most studied semiconductor materials in the field of photovoltaics 5 . Their extraordinary properties, including high carrier mobilities, low carrier recombination rates, and the tunable spectral absorption range are attributed to the unique electronic properties of these materials [5][6][7] . Thanks to the enormous interest from the scientific community, the field of hybrid perovskites has quickly expanded in terms of types of materials by substituting one or more of the organic or inorganic ions in one of the most studied perovskites, methylammonium lead iodide (CH 3 NH 3 PbI 3 ), to obtain the metal halide perovskites AMX 3 : (A = Cs, CH 3 NH 3 , CH 2 NHCH 2 , M = Sn, Pb; X = I, Br, Cl).Despite the rapid progress made in the last few years in terms of the conversion efficiency, the understanding of the fundamental electronic properties of AMX 3 perovskites is rather limited. This is especially true for realistic structures in working devices, which often are compounds with mixtures of more than one organic cation, metal cation or halide anion with sophisticated surfaces and interfaces [1][2][3][4][5][6][7] . The challenges to fundamental understanding of the electronic structure of AMX 3 ...