Uppresses the recombination of Bi2O2CO3 b , and as a result enhancing
Uppresses the recombination of Bi2O2CO3 b , and hence enhancing the photocatalytic efficiency [51]. S2 photogenerated e S2 S4 The photocurrent of pure Bi2 O2 CO3 , S2 and S4 (pure BiOI) samples S4 shown in are -7 2.0×10 Figure 8b. The photocurrent density generated by the S2 PHA-543613 Membrane Transporter/Ion Channel sample is certainly larger than that of pure Bi2 O2 CO3 and BiOI. Therefore, the PL and photocurrent measurements all demonstrate that the 1D/2D Bi2 O2 CO3 iOI heterostructure can considerably market the -7 1.0×10 separation and transfer of photogenerated electron ole pairs. To be able to receive the relative positions from the conduction band (CB) and valence band (VB) edges, VB-XPS of Bi2 O2 CO3 and S4 (pure BiOI) had been characterized (Figure 9). The 0.0 EVB major of Bi2 O2 CO3 and S4 find at 1.78 and 1.15 eV, respectively. Around the basis in the VB 500 550 600 650 700 90 position and their band gaps, the CB edge potentials of120 two OTime(s) BiOI are estimated Bi 150 three 180 210 240 2 CO and Wavelength(nm) to become -1.18 and -0.6 eV, respectively through the equation ECB = EVB .Current density(A.cm )-Figure 8. The area temperature PL spectra (ex = 320 nm) (a) and photocurrent spectra (b) of Bi2O2CO3, S2 and S4 samples.Catalysts 2021, 11,3 samples, which implies 1D/2D heterostructure effectively suppresses the recombination of photogenerated e , and thus enhancing the photocatalytic overall performance [51]. The photocurrent of pure Bi2O2CO3, S2 and S4 (pure BiOI) samples are shown in Figure 8b. The photocurrent density generated by the S2 sample is definitely greater than that of pure Bi2O2CO3 and BiOI. Therefore, the PL and photocurrent measurements all demon-12 8 of strate that the 1D/2D Bi2O2CO3 iOI heterostructure can drastically promote the separation and transfer of photogenerated electron ole pairs.Bi2O2CO3 S2 SCurrent density(A.cm )aIntensity(a.u.)-3.0x-bBi2O2CO3 S2 S2.0x-1.0x-0.0 90Catalysts 2021, 11, x FOR PEER REVIEWWavelength(nm)Time(s)9 ofFigure 8. The space temperature PL spectra (ex = 320 nm) (a) and photocurrent spectra (b) of Bi2 O2 CO3 , S2 and S4 samples. Figure 8. The area temperature PL spectra (ex = 320 nm) (a) and photocurrent spectra (b) of Bi2O2CO3, S2 and S4 samples.Intensity(a.u.)So that you can receive the relative positions of your conduction band (CB) and valence band Bi2O2CO3 (VB) edges, VB-XPS of Bi2O2CO3 and S4 (pure BiOI) have been characterized (Figure 9). The EVB top rated of Bi2O2CO3 and S4 find at 1.78 and 1.15 eV, respectively. OnS4 basis with the VB the position and their band gaps, the CB edge potentials of Bi2O2CO3 and BiOI are estimated to be -1.18 and -0.six eV, respectively by means of the equation ECB = EVB.1.15eV01.78eVBanding Power(eV)Figure 9. The VB-XPS spectra of Bi2O22 CO3and S4 (pure BiOI). The VB-XPS spectra of Bi2 O CO3 and S4 (pure BiOI).Schematic diagram for power band Bi O two O2 three iOI, the the formation from the p Schematic diagram for power band of of 2Bi2COCO3 iOI, formation in the p juncjunction the possible charge separation is displayed in Figure10. We knowknowp-n junction and and the Pinacidil Epigenetic Reader Domain doable charge separation is displayed in Figure 10. We that that p-n junctions can be formed involving (Figure 10b), The internal electric field Bi Bi 2CO3 iOI ptions can be formed in between (Figure 10b), The internal electric field of of 2O2 O2 CO3 iOI p-n heterojunction promotes the migration price of photogenerated electrons and holes, n heterojunction promotes the migration price of photogenerated electrons and holes, which drastically improves the photocatalytic ac.
