“…The common materials exploited as electron transport layer in regular configuration are generally n-type semiconductor metal oxides such as titanium dioxide (TiO 2 ), zinc oxide (ZnO), tin dioxide (SnO 2 ), whereas fullerene derivatives such as C 60 and phenyl-C 61 -butyric acid methyl ester (PCBM) are preferred in inverted configuration. Otherwise, the familiar materials involved 2,2′,7,7′-Tetrakis[N,N-di(4-methoxyphenyl)amino]-9,9′-spirobifluorene (spiro-OMeTAD), poly (3,4-ethylenedioxythiophene): poly(styrene-sulfonate) (PEDOT:PSS), poly [bis(4-phenyl)(2,4,6-trimethylphenyl) amine] (PTAA), nickel oxide (NiO x ), copper (I) iodide (CuI), copper iron oxide (CuFeO 2 ), copper chromium oxide (CuCrO 2 ), and copper thiocyanate (CuSCN) are ordinarily applied as an hole transport layer in perovskite solar cells architecture (Rashad and Shalan 2014;Elseman et al 2020Elseman et al , 2019Atabaev 2017;Olivera et al 2018;Akin et al 2019b, a;Akin et al 2018;Mudhoo et al 2020;Sengul and Asmatulu 2020;Shukla and Oturan 2015;Mohammed et al 2020). Both electron transport layer and hole transport layer are responsible for obtaining effective solar cells as the perovskite layer can absorb the light to separate the charges, the electron transfer to electron transport layer and the hole transfer to hole transport layer and when the layers work efficiently, the amount of charge separation increases and the recombination process between carriers decreases.…”