“…In this context, CO 2 photoconversion into carbon-based fuels (CO, CH 4 , and so on) is a potential approach to mitigate the greenhouse effect and energy crisis . Among these carbon-based fuels, CO 2 photoreduction into CH 4 has attracted attention in academia and industry, since CH 4 with a calorific value of 890 kJ mol –1 can be utilized to directly fabricate chemical products and act as a living fuel. , However, the ultrahigh stability of CO 2 (the dissociation of CO = 750 kJ mol –1 ) results in a high energy barrier of CO 2 activation in thermodynamics, and hence CO 2 photoreduction into CH 4 encounters very poor activity. , Furthermore, the formation of CH 4 requires eight electrons, which is kinetically unfavorable compared to the generation of CO (two electrons), causing the generation of byproducts in the kinetics. − In this case, CO 2 photoreduction into CH 4 on traditional semiconductors suffers from low efficiency and unwanted byproducts due to the poor light absorption, slow charge separation efficiency, and surface reduction reaction. , Given this, many reports employ the broad-bandgap semiconductor to improve the efficiency of electron and hole separation for boosting the high-rate CO 2 reduction into CH 4 . Unfortunately, in the view of thermodynamics, the broad-bandgap semiconductor, such as ZnO, TiO 2 , and Ga 2 O 3 , usually can simultaneously match the reduction potential of various products, such as E CO2/CH4 = −0.24 V vs. NHE = 7 and E CO2/CO = −0.53 V vs. NHE = 7, resulting in uncontrollable selectivity. , In this case, construction of the cocatalyst (loading metal particle or metal oxides particles) helps to adjust the electronic structure of the semiconductor to narrow the distribution of products. − Nevertheless, as for these architectures, the presence of abundant microscopic structures causes it unable to determine the active species .…”