“…PSC architecture is quite simple in its standard configuration:aconductive glass (or plastic foil) supports an electron extraction layer (like TiO 2 or SnO 2 [13] ), on top of which the perovskite-active material is deposited.Ahole-transporting material (HTM) is coated above the perovskite layer,a nd gold backcontactsa re evaporated on the top of the cell. [14][15][16][17] Sunlight absorption leads to charge-generation, and both negative and positivec hargec arriers are transported through the perovskite to charges electivec ontacts.T he core of this device is the perovskitel ayer,b earing ag eneric structure ABX 3 ,i nw hich Ai sa monovalentc ation (like methylammonium CH 3 NH 3 + ,f ormamidinium CH 2 (NH 2 ) 2 + ,C s + ,R b + ), Bs tands for Pb II or Sn II and X for Io rB r. [18] The successo ft his materials is given by its outstanding optoelectronic properties,m erging high absorption coefficient and mobility,l ow exciton binding energy and long balanced carrier diffusion length; [19][20][21][22][23] moreover,t he device can also work in the inverted configuration. [24] Several review articles have been published on strategies to improve the performance of laboratory-scale PSCs.…”