Thermalization of photogenerated HCs occurs by dissipating their excess energy as heat energy through phonons which is the major intrinsic loss channel for solar cell devices. [3] Harnessing the excess energy of photoexcited HCs will allow us to achieve maximum power conversion efficiency (PCE) up to 67% for a single-junction solar cell under one sun illumination, [4] breaking the socalled Shockley-Queisser (SQ) limit of 34%. [5] Photoexcited HCs are used in photo-catalysis, photodetection, and highpower optoelectronic devices to improve efficiency. [6,7] However, rapid energy loss mechanisms of HCs in most of the conventional semiconductor nanomaterials (e.g., GaAs, PbSe, InN, and CdSe) through carrier-phonon scattering processes in sub-picosecond timescale severely restrict the utilization of non-thermalized excess energy of photo-excited HCs. [8][9][10][11] Therefore, it is essential to develop a solar absorber with retarded HC cooling rate. [12,13] Due to their extraordinary performance, metal halide perovskite nanocrystals (NCs) have recently emerged as front-runner materials in low-cost, high-performance solar cells. [14][15][16] A lot of interest has been shown to understand the HC cooling dynamics of lead halide perovskite (LHP)to find out potential applications. [17][18][19][20][21] Slow HC relaxation mechanisms in perovskite materials are reported due to the hot-phonon bottleneck effect, [22] Auger-heating effect, [23] band-filling effects, [24] dielectric screening, [25] and significant polaron screening effects. [26] However, in most cases, high pump fluence with photo-excited carrier densities of 10 18 -10 19 cm −3 was used, which is hard to accomplish in practical conditions. [22,27] It is worth noting that HC relaxation of LHP still occurs very rapidly (within hundreds of femtoseconds) under weak carrier densities (comparable to sun illumination level, ≈10 17 cm −3 ). [28,29] Thus, slowing down the HC relaxation rate of halide-based perovskite materials under low excitation power densities is a challenge for hotcarrier-based optoelectronic applications. Recently, delayed HC cooling rate has been reported in CsPbBr 3 based asymmetric multiple quantum wells (MQWs) due to sequential hot-electron transfer between CsPbBr 3 layers. [30] Tuning the HC cooling dynamics of metal halide perovskite is mainly limited to reduction of dimensionality, [31] changing cation/ halide ions, [32][33][34] and doping impurity ions. [35] Therefore, significant efforts are Metal halide perovskite nanocrystals have recently emerged as a front-runner material for high-performance solar cells. However, slowing down the hot carrier (HC) cooling of perovskites at carrier densities comparable to the sun-illumination level (≈10 17 cm −3 ) is still a thriving challenge. A new strategy is presented to retard the HC cooling via charge localization at the CsPbBr 3 / PbSe heterostructure interface. Ultrafast transient absorption study reveals two times slower HC relaxation time (from 770 fs to 1.4 ps) and much higher initial HC temper...