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Graphene-based nanomaterials for solar cells                      143

           for DSSCs with an efficiency of 6.75% [127]. The high efficiency was attributed to the
           uniform distribution of catalytic Fe particles on the surface of the HRG. Recently, gold
           metal-incorporated,  graphene-based  composites on  FTO substrate  used as  counter
           electrodes in DSSCs have achieved a record efficiency of 14.3%.

           7.4.6   Graphene in perovskite solar cells (PSC)

           Perovskite solar cells emerged as a new family of solar cells during the past decade.
           They are third-generation solar cell and are attractive candidates for future commer-
           cialization because of their low-cost, ability to scale up, and high power conversion ef-
           ficiency (more than 20%). Similar to DSSCs, PSCs consist of semiconducting TiO 2  as
           an electron-transport layer, perovskites as light harvesting materials, a hole transport
           layer, and an electrode. Various perovskites, for example, CH 3 NH 3 PbI 3 , CH 3 NH 3 PbB 3 ,
           and NCs, are being used in place of dyes in DSSCs [128]. In PSCs, graphene-based
           materials are commonly applied as an electron transport layer or a hole transport layer
           Fig. 7.3 illustrates the arrangement of perovskite solar cells.
              Recently, HRG-TiO 2  nanocomposites were used as an electron transport layer in
                                                                         2
           PSCs and exhibited a maximum PCE of 15.6% with a JSC of 21.9 mA/cm . Also,
           graphene quantum dots were introduced between the perovskite and TiO 2  to enhance
           the performance of the PSC. In this case, a PCE of 10.15% was achieved, which is
           higher than in a PSC without a GQD layer [129]. In addition, binary or ternary oxides
           such as SrTiO 3  are considered as suitable alternatives to TiO 2  as ETLs [130]. These
           materials decreased charge recombination centers and therefore improved the PCE to
           10%. Wu et al. reported inverted planar heterojunction perovskite-based solar cells
           using GRO as a hole conductor and CH 3 NH 3 PbI 3−x Cl x  as a light absorber [70]. The
           deliberately designed device exhibited a high efficiency of 12.4%. In another study,
           ultrathin HRG was used as the hole transport material with CH 3 NH 3 PbI 3  as a light ab-
           sorber. The PCE of rGO-based PSC was 10.80% and also showed better stability than
           a PEDOT:PSS device (maximum PCE, 9.14%) [131].




                                   Perovskite solar cell

                                                 Graphene
                         Counter electrode
                                                 Graphene-based material
                         Hole transport layer    Graphene-based nanocomposite
                           Perovskite layer

                               TiO 2
                              FTO glass          Graphene-based material





           Fig. 7.3  Graphene-based material used in perovskite solar cells.
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