large organic ligands with the formula of A 2 A′ n−1 M n X 3n+1 . [9][10][11][12] Such 2D perovskites can demonstrate remarkable tunabilities on optical properties via controlling morphological structures by selecting different functional A/A′ molecules. [13][14][15] Through down-conversion excitation, 2D perovskites have shown efficient light emission in spontaneous [16,17] and stimulated [18,19] regimes. Recently, amplified spontaneous emission (ASE) have been reported in 2D perovskites [(NMA) 2 (FA)Pb 2 Br 7 and (NMA) 2 (FA)Pb 2 Br 1 I 6 ] with stoichiometrically tunable wavelength from visible to near-infrared spectral range (530-810 nm) with the gain coefficient as high as > 300 cm −1 under pulse laser excitation. [20] On the other hand, it has been found that the edge states can be formed in 2D perovskites with light-emitting properties below the bandgap. [21] The discovery of edge states triggers a fundamental question of whether the gap states can be introduced as a new approach to develop multi-photon up-conversion light emission in solution-processing quasi-2D perovskite films. We should note that an up-conversion ASE was indeed observed at 720 nm in inorganic 3D perovskite (CsPbI 3 ) nanoplates under the infrared pulse laser excitation of 1200 nm. [22] In this work, we explore a new approach to realize multi-photon up-conversion photoluminescence (PL) in quasi-2D perovskite [(PEA) 2 (MA) 4 Pb 5 Br 16 (n = 5)] films by directly exciting broad gap states with continuous-wave (CW) infrared photoexcitation. The broad gap states were adjusted by selecting different n values (n = 1-5) with accelerated crystallization in quasi-2D perovskite films prepared with antisolvent processing method. Here, we found that an up-conversion PL can be observed in 2D perovskite [(PEA) 2 (MA) 4 Pb 5 Br 16 (n = 5)] films under CW 980 nm excitation when broad infrared absorption is appeared between 800 and 1500 nm. To further understand the up-conversion PL under CW infrared excitation, magnetic field effects of PL (namely, magneto-PL) were used to identify whether the gap states function as spatially extended states to generate multiphoton absorption in quasi-2D perovskite films. Furthermore, polarization-dependent PL upon using linearly and circularly polarized photoexcitations was used to explore the effects of orbit-orbit interaction on multi-photon up-conversion PL under A new approach to generate a two-photon up-conversion photoluminescence (PL) by directly exciting the gap states with continuous-wave (CW) infrared photoexcitation in solution-processing quasi-2D perovskite films [(PEA) 2 (MA) 4 Pb 5 Br 16 with n = 5] is reported. Specifically, a visible PL peaked at 520 nm is observed with the quadratic power dependence by exciting the gap states with CW 980 nm laser excitation, indicating a two-photon up-conversion PL occurring in quasi-2D perovskite films. Decreasing the gap states by reducing the n value leads to a dramatic decrease in the twophoton up-conversion PL signal. This confirms that the gap states are indeed ...