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Metal-based semiconductor nanomaterials for photocatalysis        203

           processes and sintering damage, which reduces the surface area and could also cause
           a phase transition of the material (i.e., anatase to rutile).
              The activity is dependent on the amount and the loading method of the co-catalyst
           (i.e., zero-valent metal) on the base photocatalyst. Highly dispersed nanoparticles of
           co-catalyst contribute to increasing the rate of hydrogen production, but excess load-
           ing reduces the catalytic activity because it hinders the radiation absorption and, in
           some cases, can favor the recombination process between electron-hole pairs [125].
           Therefore an optimum load of co-catalyst can be found to maximize the catalyst ac-
           tivity (Fig. 9.11).
              Moreover, the increase in loading determines the increase in reaction rate. However,
           there is also a limiting load for the base photocatalyst, above which hydrogen produc-
           tion rate does not further increase because of particle agglomeration and radiation
           shadowing phenomena for high turbidity of particles’ suspensions [126].
              The pH of the solution is an additional important variable to be controlled because
           it affects both the stability of materials and the photocatalytic process. For exam-
           ple, the rates of water photosplitting are favored under alkaline pH conditions in the
           presence of NiO x -loaded perovskites [87,127,128] and in acidic pH conditions using
           RuO 2 -loaded oxynitrides [129,130]. Even in the presence of the same base photocat-
           alyst, the optimal pH conditions differ depending on the co-catalyst used because of
           corrosion and hydrolysis phenomena [129,131]. Changes in pH of the solution could
           also affect the position of the band-edge potential of the photocatalyst [132,133].






                    •  Increase charge carriers separation  •  Lower density of  photoactive sites of
                    •  Higher absorption in visible light    base material
                     range                         •  Change of  polar characteristics of
                    •  Lower overpotential of  redox    photocatalyst surface
                     reactions                     •  Occurring of  aggregation phenomena
                   Photocatalyst activity












                      Poor load of cocatalyst  Excessive load of cocatalyst

                                       Loading of cocatalyst
           Fig. 9.11  Effect of co-catalyst loading on the photocatalyst activity.
           Adapted from K. Maeda, Photocatalytic water splitting using semiconductor particles: history
           and recent developments, J. Photochem. Photobiol. C Photochem. Rev. 12 (2011) 237–268.
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