All‐inorganic lead‐free halide perovskites have been at the forefront of state‐of‐the‐art optoelectronic materials due to their impressive optoelectronic properties and straightforward solution processability. The exceptional optical properties of halide perovskites are intrinsically linked to their structural characteristics, making the investigation of structure–property relationships critical for advancing functional material design and optimizing performance in optoelectronic applications. Among various tuning methods, pressure engineering is a highly powerful in situ technique, which can efficiently modulate the structural and optical properties. The pressure‐induced structural transitions of all‐inorganic lead‐free halide perovskite lead to significant bandgap engineering, piezochromic behaviors, and emission enhancements. However, systematic and comprehensive reviews in this field remain scarce. In this review, recent progress on studies on pressure effect on all‐inorganic lead‐free halide perovskite materials is summarized. The underlying mechanisms of pressure effects on these materials are discussed comprehensively. Finally, the current review challenges and offers insights into the future prospects for leveraging pressure effects to further develop perovskite structures and properties.
The toxicity of lead in conventional perovskites and their inherent chemical instability impede the commercialization of perovskite-based optoelectronics. Therefore, it is vital to develop chemically stable and environmentally friendly Pb-free alternatives. Recently, zero-dimensional (0D) all-inorganic Cs2ZnCl4 doped with Sn(II) has emerged as a promising candidate, exhibiting superior chemical robustness, minimal biotoxicity, and exceptional optoelectronic properties. In this work, pressure effects on structure and optical properties in Sn(II)-doped all-inorganic zero-dimensional halide perovskite are investigated both experimentally and theoretically. The structure–property relationship of Sn(II)-doped Cs2ZnCl4 is studied using high-pressure techniques. Piezochromism, accompanied by a remarkable change in emission color from orange/red and green to orange/yellow, was obtained from 1 atm to 22.5 GPa. Angle dispersive synchrotron X-ray diffraction (ADXRD) patterns and Raman spectra manifest that the material underwent an isostructural phase transition followed by amorphization with increasing pressure. The piezochromism and band gap engineering originate from the pressure-induced lattice compression and isostructural phase transition. This work advances STE emission studies and provides a robust strategy to boost emission efficiency and to construct multifunctional materials with piezochromism in environmentally friendly perovskites, thus facilitating diverse future applications.
Lead-free perovskite variants have emerged as promising candidates due to their self-trapped exciton emission. However, in ASnX3 systems, facile oxidation of Sn(II) to Sn(IV) yields A2SnCl6 vacancy-ordered derivatives. Paradoxically, despite possessing a direct bandgap, these variants exhibit diminished photoluminescence (PL). Doping engineering thus becomes essential for precise optical tailoring of A2SnX6 materials. Herein, through integrated first-principles calculations and spectroscopic analysis, we elucidate the luminescence mechanism in Te4+-doped (NH4)2SnCl6 lead-free perovskites. Density functional theory, X-ray diffraction (XRD) patterns and X-ray photoelectron spectroscopy (XPS) confirm Te4+ substitution at Sn sites via favorable chemical potentials. Spectral interrogations, including absorption and emission profiles, reveal that the intense emission originates from the triplet STE recombination (3P1 → 1S0) of Te centers. Temperature-dependent PL spectra further demonstrate strong electron–phonon coupling that induces symmetry-breaking distortions to stabilize STEs. Complementary electronic band structure and molecular orbital calculations unveil the underlying photophysical pathway. Leveraging these distinct thermal responses of PL intensity and peak position, 0.5%Te:(NH4)2SnCl6 emerges as a highly promising candidate for non-contact, dual-parameter optical thermometry over an ultra-broad range (100–400 K). This work provides fundamental insights into the exciton dynamics and thermal engineering of optical properties in this material system, establishing its significant potential for advanced temperature-sensing applications.