Organic-inorganic metal halide perovskites are superstars for photovoltaics and optoelectronics due to their excellent defect tolerance, high charge mobility, tunable optical bandgap, and high absorption coefficient. [1-3] In fact, their power conversion efficiency (PCE) has been increased from 3.8% to 25.2% in just a few years. [4-6] Unfortunately, the organic components in the perovskite composition make them susceptible to stressing conditions including high temperature, chemical, and ultraviolet radiation. [7-10] Inorganic cesium halide perovskites (CsPbX 3 , X ¼ I or Br) without the organic component are attractive in the long run because of their advantages in thermal stability, and chemical resistance. [11-13] CsPbI 3 possesses an attractive bandgap of %1.73 eV to absorb most of the solar energy in visible spectrum; PSCs based on CsPbI 3 have achieved champion efficiencies as high as 19.03%. [14] Unfortunately, the desired PV active α-phase CsPbI 3 is not thermodynamically stable at room temperature. It can be easily transitioned to PV-inactive yellowish δ-phase. Such conversion leads to a considerable drop in PCE and stability. [15,16] Extensive efforts have been devoted to address these issues. Bromine has been used to partially or even completely substitute iodine in the CsPbX 3 composition. For example, a PCE of over 16% has been achieved for CsPbI 2 Br PSCs with relatively enhanced stability. [17,18] Furthermore, a PCE of 10.79% has been attained for CsPbBr 3-based PSCs with an extraordinarily high open-circuit voltage exceeding 1.6 V and decent stability upon Sm 3þ ion doping. [19] Nevertheless, its wide bandgap of %2.3 eV leads to reduced capability of solar light harvesting, which in turn limits its application. [20]