MHPs have also recently been actively studied for use in multijunction cells in association with other conventional solar cells, such as CuInGaS(e) (CIGS(e)), organic photovoltaic (OPV), quantum dot (QD), and c-Si solar cells. [14-18] Multijunction solar cells that employ more than two light-absorbing materials have long been in development to overcome the theoretical PCE limit of single-junction solar cells, also known as the Shockley-Quiesser (SQ) limit, of 31.1% under 1 sun. [19,20] The theoretical PCE limit for a single-junction cell originates from thermalization and transmission losses, [21] both of which can be reduced by employing multiple junctions between materials with different bandgaps. Thermalization losses occur due to the difference in energy between the absorbed photon and the bandgap of the light absorber, while transmission losses occur due to nonabsorbed photons with a lower energy than the bandgap. Therefore, in a tandem cell, the monolithic connection of a lightabsorbing top layer with a wide bandgap and a light-absorbing lower layer with a narrow bandgap reduces thermalization and transmission losses, respectively. Multijunction cells can theoretically achieve extremely high PCEs, but related research has been limited to certain solar cells that use III-V semiconductors as light-absorbing materials. In tandem solar cells, the higher the number of light absorbers with different bandgaps that are employed, the greater the theoretical PCE that can be achieved. For example, III-V multijunction solar cells with a nonconcentrator and two, three, or six junctions currently achieve PCEs of 32.9%, 37.9%, and 39.2%, respectively. [12] GaInP/GaAs monolithic two-junction cells are a common example of this type of cell. To produce high-performance tandem cells, the bandgap of the light absorbers should be tunable, and high PCEs should be achievable within every single cell with the desired bandgap. III-V semiconductors satisfy these requirements, with a bandgap that is broadly tunable via the compositional engineering of Ga 1−x (In) x As 1−y (P) y (0 ≤ x, y ≤ 1) and epitaxially grown highly crystalline film that allows high PCEs to be realized for these engineered composite materials. This is why previous studies on multijunction cells have been limited to III-V solar cells. However, the required metal-organic chemical vapor deposition process is expensive, and a singlecrystal substrate is essential for the growth of the epitaxial film, thus limiting the commercial practicality of III-V tandem cells for use as terrestrial solar cells or as part of other photovoltaic systems. MHP solar cell technology has the potential to overcome the high cost of tandem cells. MHPs demonstrate optoelectronic Metal halide perovskite (MHP)-based tandem solar cells are a promising candidate for use in cost-effective and high-performance solar cells that can compete with fossil fuels. To understand the research trends for MHPbased tandem solar cells, a general introduction to single-junction and multiple-junction MHP solar ...