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Graphene photocatalysts                                            93

             tourmaline co-doped TiO 2  nanocomposites (GT/T) [115]. GT/T exhibited significantly
           improved activity compared to the graphene-loaded TiO 2 , tourmaline-loaded TiO 2 ,
           and bare TiO 2 . This enhancement was attributed to the synergistic effect of graphene
           and tourmaline. Specifically, both graphene and tourmaline can improve electron-hole
           separation, whereas graphene can reduce the band gap of TiO 2 . As a result, GT/T led
           to the enhanced MeOH production rate via photocatalytic CO 2  reduction, which was
           21 times higher than that of bare TiO 2 .
              A well-defined nanocomposite interface, such as a 2D–2D composite, is import-
           ant in preparing highly efficient graphene-based photocatalysts [110]. Robust hollow
           spheres  consisting  of  molecular-scale  alternating  titania  (Ti 0.91 O 2 )  nanosheets  and
           graphene nanosheets were used for the photocatalytic reduction of CO 2  using a 300
           W Xe arc lamp [116]. Because both TiO 2  and graphene nanosheets are 2D struc-
           tures, graphene and Ti 0.91 O 2  had a close and large contact surface area. The prepared
           samples exhibited a high CO formation rate via the photocatalytic CO 2  reduction,
           which was nine times higher than that of the commercial P25, because of its fast
           electron- hole separation and good light utilization. 2D-2D layered photocatalysts
           based on sandwich-like graphene-g-C 3 N 4  (GCN) composite showed enhanced visible
           light photocatalytic CO 2  reduction activity [96]. The GCN sample demonstrated high
           visible- light photoactivity toward CO 2  reduction under ambient conditions, exhibiting
           a 2.3-fold enhancement over bare g-C 3 N 4  (Fig. 5.9A). This effect was ascribed to the
           inhibition of the electron-hole pair recombination by graphene, which increased the
           charge transfer (Fig. 5.9B).
              Nonmetal doping is another efficient way to tune the physical, optical, and phys-
           icochemical  properties  of  graphene  for  photoreduction  of  CO 2 .  Boron  (B)-doped
           graphene (B-GR) nanosheets loaded on P25 nanoparticles have been proposed to im-
           prove the photocatalytic reduction of CO 2  using a 300 W Xe lamp as the light source
           [101]. B-GR showed a higher Fermi level than pristine graphene, falling between the
           CB of P25 and the relevant CO 2 /CH 4  redox potential. The tunable band gap of B-GR
           determined the large potential application of P25/B-GR in the photoreduction of CO 2 .














           Fig. 5.9  (A) Total CH 4  yield over the as-prepared photocatalysts; (B) schematic diagram of
           photogenerated charge transfer in the GCN system for CO 2  reduction with H 2 O to form CH 4
           under visible light.
           Reproduced with permission from W.-J. Ong, L.-L. Tan, S.-P. Chai, S.-T. Yong, Graphene
           oxide as a structure-directing agent for the two-dimensional interface engineering of
           sandwich-like graphene-g-C3N4 hybrid nanostructures with enhanced visible-light
           photoreduction of CO 2  to methane, Chem. Commun. 51 (5) (2015) 858–861. Copyright 2014,
           Royal Society of Chemistry.
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