Perovskite light-emitting diodes (PeLEDs) own great attention in recent years, due to their narrow emission bandwidth and tunable emission spectrum. E cient red emission is one of most important part for lighting and display. Quasi-two-dimensional (quasi-2D) perovskite could deliver high emission e ciency due to the strong carrier con nement, while the external quantum e ciencies (EQE) of red quasi-2D PeLEDs are ine cient at present, which is due to the complex distribution of different n-value phases in quasi-2D perovskite lms. Here, we nely control the phase distribution of the quasi-2D perovskite by mixing two different large organic cations, which effectively reduce the amount of smaller n index phases, meanwhile the passivation of lead and halide defects in perovskite lms is realized.Accordingly, the PeLEDs showed 25.8% EQE and 1300 cd•m-2 maximum brightness at 680 nm, which exhibit the highest performance for red PeLEDs up to now.
Full TextSolution-processed metal halide perovskites have attracted considerable research interest as a new type of semiconductor materials, which has been utilized in solar cells, light-emitting diodes and other optoelectronic devices [1][2][3][4][5][6][7][8] . In particular, Perovskite light-emitting diodes (PeLEDs) have been conferred as the cutting-edging research due to their high performance [9][10][11][12][13][14][15][16] , red emission is very important in the eld of lighting and display. To date, the red PeLEDs have achieved signi cant external quantum e ciencies (EQE) that over 20%, most of them are based on the three-dimensional (3D) and quantum-dot (QD) perovskite material [17][18][19][20][21][22] .Compared with 3D and QD perovskite, quasi-two-dimensional (quasi-2D) perovskite could be more e cient emission material due to its higher exciton binding energy, multi-quantum-well structure and good charge transfer properties [23][24][25][26][27][28] . Ruddlesden-Popper perovskite (RPP) is generally described by the formula of L 2 A n-1 B n X 3n+1 as typical quasi-2D perovskites, which consist of large organic cation L, a small organic or cesium cation A, divalent metal cation B (lead or tin), and halide anion X (Cl -, Bror I -).Although the overall development of red LED is remarkable, the quasi-2D red LEDs are still in arrears of e ciency. The reason may be that ne control of quasi-2D perovskite phase (represents the thickness of the [PbI 6 ] 4octahedra layers capped by the L cations [28][29][30][31] ) distribution is a great challenge, which make the inferior charge injection and serious non-radiative recombination.In this work, we report a general strategy of cospacer cations to control the phase distribution in RPP lms, by mixing a representative of phenethylammonium iodide (PEAI)/ 3-uorophenylethylammonium iodide (m-F-PEA) and 1-naphthylmethylammonium iodide (NMAI) to alloy the RPP lms. These RPP lms show signi cant suppression of small index phase (n=2), and the carrier transport has been improved effectively. At the same time, the mixing of NMA can reduce the metall...