2023
DOI: 10.3390/mi14030639
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Study on g-C3N4/BiVO4 Binary Composite Photocatalytic Materials

Abstract: Recent studies have shown that the composite of semiconductor photocatalytic materials and g-C3N4 can effectively inhibit photocatalytic carrier recombination and enhance the adsorption performance of the composite photocatalytic materials, so that the composite photocatalyst has stronger photocatalytic activity. In this paper, three kinds of graphitic carbon nitride photocatalyst g-C3N4 with different morphologies were prepared using the same precursor system by the chemical cracking method. After characteriz… Show more

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Cited by 10 publications
(4 citation statements)
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“…9a, the fluorescence spectra of nano TiO 2 , LMO and T/LMO at an excitation wavelength of 400 nm show an obvious emission peak in the scanning range of 500–700 nm, and the fluorescence intensity is inversely proportional to the photogenerated electron–hole recombination efficiency of the material. The more the photogenerated carrier recombination, 54 the more unfavorable the degradation of ammonia nitrogen. Due to the high rate of photogenerated electron carrier complexation, the fluorescence intensity of nano-TiO 2 was the strongest with the highest peaks, while the highest peak intensity of T/LMO was significantly lower than that of monomer materials, indicating that the synthesised composites greatly suppressed the rate of electron–hole pair complexation exhibiting an improved photocatalytic performance.…”
Section: Resultsmentioning
confidence: 99%
“…9a, the fluorescence spectra of nano TiO 2 , LMO and T/LMO at an excitation wavelength of 400 nm show an obvious emission peak in the scanning range of 500–700 nm, and the fluorescence intensity is inversely proportional to the photogenerated electron–hole recombination efficiency of the material. The more the photogenerated carrier recombination, 54 the more unfavorable the degradation of ammonia nitrogen. Due to the high rate of photogenerated electron carrier complexation, the fluorescence intensity of nano-TiO 2 was the strongest with the highest peaks, while the highest peak intensity of T/LMO was significantly lower than that of monomer materials, indicating that the synthesised composites greatly suppressed the rate of electron–hole pair complexation exhibiting an improved photocatalytic performance.…”
Section: Resultsmentioning
confidence: 99%
“…As the two different semiconductor particles are coupled, the Fe-g-C 3 N 4 /Bi 2 MoO 6 composite sample has an absorption edge at 487.8 nm, showing a slight red shift. The optical bandgap energy of the prepared semiconductor samples can be calculated using the following Tauc relation [ 22 , 23 ]: α(hv) = A (hv − E g ) 1/2 , where hv is the photon energy, A is a constant, and α and E g are the absorption coefficient and the optical bandgap energy (at wave vector k equal to zero) of the semiconductors. Tauc plots are based on the relationship between (αhv) 2 and hv to determine the optical bandgap energy for direct transitions.…”
Section: Resultsmentioning
confidence: 99%
“…As the two different semiconductor particles are coupled, the Fe-g-C 3 N 4 /Bi 2 MoO 6 composite sample has an absorption edge at 487.8 nm, showing a slight red shift. The optical bandgap energy of the prepared semiconductor samples can be calculated using the following Tauc relation [22,23]:…”
Section: Physical Properties Of Semiconducting Nano-photocatalystsmentioning
confidence: 99%
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