applications, [6] X-ray detectors, [7] potential color conversion layers in visible light communication, [8,9] and mini and micro light-emitting diode (mini-and micro-LED) displays. [10][11][12] Among them, the CsPbI 3 processes the lowest bandgap, which attracts a vast interest from the community. [13] It absorbs the largest portion of solar light in solar-cells, compared to its counterparts; [14] it emits the deepest red light, constituting the largest gamut in the micro-LED display; [12,15] however, it is the least stable member of the lead-halide PNCs family. In addition to the degradation induced by external factors, which are shared among all PNCs, [11] the CsPbI 3 suffers undesirable intrinsic phase transition when the temperature is changing. So far, four phases of CsPbI 3 have been identified. They fall into two categories. The first category, being of the perovskitetype and fluorescently active, contains three phases: α (cubic), β (tetragonal), and γ (orthorhombic) phases. These three phases are collectively denoted as "black" phases. On the contrary, the second category, the "yellow" phase -δ-CsPbI 3 (non-perovskite type), is fluorescently inactive, due to its indirect bandgap. In ambient room temperature (RT), it has been proven that the γ-CsPbI 3 exhibits the highest stability among three black phases, but is still less stable than the thermodynamically favored δ-CsPbI 3 . [16] Phase transitions can be observed at changing temperature, as sketched in Figure 1. At 1 atm, the CsPbI 3 exists in the form of α phase when the temperature is higher than 320 °C, but this critical temperature depends on the pressure. [17] Upon cooling, the CsPbI 3 PNCs either turn directly into δ phase, in the case when no constraint or pressure is exerted, [17,18] as sketched in the Route (1) in Figure 1, or into β and γ phases in succession and temporarily maintains in black phase at RT, in cases where there exist constraints of proper degree [17,19] or crystal grains are sufficiently small, [4] as sketched by Route (2) in Figure 1, but under some triggers, such as environmental humidity in ambient, the meta-stable γ-CsPbI 3 would eventually turn into δ-CsPbI 3 (Route (3), Figure 1). [13,17,20] During heating, if starting from the yellow phase at RT, the δ-CsPbI 3 phase turns to α-CsPbI 3 when the temperature approaches the range from 300 to 450 °C (route (4), Figure 1). [17,[21][22][23] If starting from the black phases at RT (commonly γ-CsPbI 3 ), although it would end up α-CsPbI 3 at temperatures beyond 300 °C, according to literature published, the γ-CsPbI 3 will first transfer to δ-CsPbI 3 This work combines the high-temperature sintering method and atomic layer deposition (ALD) technique, and yields SiO 2 /AlO x -sealed γ-CsPbI 3 nanocrystals (NCs). The black-phase CsPbI 3 NCs, scattered and encapsulated firmly in solid SiO 2 sub-micron particles, maintain in black phases against water soaking, ultraviolet irradiation, and heating, exhibiting remarkable phase stability. A new phase-transition route, from γ via β to α ...