“…Recently, dibismuth dioxychalcogenides, Bi 2 O 2 Ch (Ch = S, Se, Te), and their 2D counterparts − have garnered tremendous research interest due to their potential applications in thermoelectrics, ,, ferroelectrics, and optoelectronics. ,,− Bi 2 O 2 (Se/Te) crystallizes in the body-centered tetragonal (SG: I 4/ mmm , Z = 1 formula units (fu) per primitive cell) anti-ThCr 2 Si 2 -type structure, while Bi 2 O 2 S prefers to crystallize in the low-symmetry primitive orthorhombic structure (SG: Pnmn , Z = 2 fu) per primitive cell) due to the stereochemically active 6s 2 lone pair of Bi 3+ cations. The stereochemically active lone pair creates a structural distortion, causing a material to crystallize in relatively low symmetry compared to materials with stereochemically inactive lone pairs. , The crystal structure of Bi 2 O 2 Ch consists of alternating Bi 2 O 2 and chalcogen (S/Se/Te) layers, which are held together by strong electrostatic forces , in contrast to van der Waals (vdW) interactions that are typically observed in layered materials. − Infrared, Raman spectra, and strain effects on bulk and monolayer Bi 2 O 2 Ch crystals have been systematically investigated to explore their possible applications in nanoelectronics …”