“…[ 4–7 ] This is attributed to their favorable optoelectronic properties, such as large exciton binding energy, [ 8 ] sizeable oscillator strength, [ 9 ] robust chemical stability, [ 5 ] as well as facile photophysical tunability, etc. Despite the inroads in understanding various phenomena, such as spin‐selective optical Stark effect, [ 10 ] image charge effect, [ 8,11 ] and Rashba splitting [ 12 ] etc., progress remains modest for carrier–phonon coupling that significantly affects the optical and electronic properties of the 2D halide perovskites, such as absorption and photoluminescence (PL) line shape, [ 13,14 ] carrier recombination, [ 15 ] and hot carrier cooling, [ 16–18 ] etc. Although experimental observations of electron–phonon coupling are well reported, how these lattice vibrations modulate the optical properties of the halide perovskites is still an open question.…”