“…[ 4 ] More importantly, the unique 2D layered crystal structure that organic and inorganic layers self‐assemble alternately in the direction perpendicular to a substrate enables charge carriers to transport in the inorganic frameworks, resembling the lateral transport behavior in field‐effect transistors. [ 5 ] The most common 2D layered perovskite materials currently used in transistors are Sn‐based perovskites, such as phenylethylammonium tin iodide perovskite ((PEA) 2 SnI 4 ) and its derivatives, [ 6 ] 2‐(3′″,4′‐dimethyl‐[2,2′:5′,2″:5″,2′″‐quaterthiophen]‐5‐yl)ethan‐1‐ammonium tin perovskite ((4TM) 2 SnI 4 ), [ 7 ] butylammonium tin iodide perovskite ( n ‐BA 2 SnI 4 ), [ 8 ] (PEA) 2 (FA) n −1 Sn n I 3 n +1 ( n = 4, 8; FA: formamidinium), [ 9 ] and (PEA) 2 CsSn 2 I 7 (Cs: cesium), [ 10 ] while very few studies have been focused on 2D Pb‐based perovskite field‐effect transistors. [ 3c,11 ] Among them, (PEA) 2 SnI 4 is the first hybrid perovskite material applied to transistors, [ 6a ] and a record‐breaking hole mobility of 15 cm 2 V −1 s −1 has been achieved in the (PEA) 2 SnI 4 field‐effect transistors in vacuum at room temperature.…”