TY - JOUR
T1 - Slow Light Effect Enhances the Photocatalytic Effect of Inverse Opal TiO2-Based Photonic Nanocrystals
AU - Zhang, Jiaojiao
AU - Cai, Xiaolu
AU - Fu, Xuewen
AU - Teng, Da
AU - Murtaza, Ghulam
AU - Meng, Zihui
AU - Jia, Zhiyu
AU - Qiu, Lili
N1 - Publisher Copyright:
© 2024 American Chemical Society.
PY - 2024/7/12
Y1 - 2024/7/12
N2 - The slow light effect at the band gap edge of photonic nanocrystals (PhCs) can improve the light utilization efficiency of photocatalysts by enhancing light collection. This study reported an anatase inverse opal TiO2 (IO TiO2) with a 3D closely packed face-centered cubic structure prepared using a PhC template. The simulation of the electric field modulus distribution in the inverse opal structure was performed, and the enhancement of photocatalytic efficiency caused by the slow light effect at the red and blue edges of the photonic band gap was analyzed. The experimental results of rhodamine B degradation agreed with the simulation. IO TiO2 has a high specific surface area (91 m2/g), which is 4.33 times that of powder TiO2, and also has high pore volumes (0.13 cm3/g). In addition, it facilitates the separation of photogenerated carriers due to the existence of large pores that are periodically interconnected, thus, significantly improving photocatalytic efficiency. The apparent rate constant of IO TiO2 is 9.96 × 10-3 min-1, which is 1.81 times that of powder TiO2. The blue edge of 200 nm IO TiO2 is spectrally closer to the electronic band gap of TiO2. Also, it presents optimal photodegradation efficiency (70.02%), and its rate constant is 2.13 times higher than porous block TiO2 without a band gap. Moreover, a detailed path of a possible reaction mechanism is proposed based on the results of the free radical trapping experiment and EPR analysis. This research offered opportunities for a deeper understanding and more efficient utilization of the blue-edge slow light effect. The slow light can be leveraged to enhance the optical nonlinear effect, which has practical significance for solar energy collection and conversion, optical switches, and photocatalysis.
AB - The slow light effect at the band gap edge of photonic nanocrystals (PhCs) can improve the light utilization efficiency of photocatalysts by enhancing light collection. This study reported an anatase inverse opal TiO2 (IO TiO2) with a 3D closely packed face-centered cubic structure prepared using a PhC template. The simulation of the electric field modulus distribution in the inverse opal structure was performed, and the enhancement of photocatalytic efficiency caused by the slow light effect at the red and blue edges of the photonic band gap was analyzed. The experimental results of rhodamine B degradation agreed with the simulation. IO TiO2 has a high specific surface area (91 m2/g), which is 4.33 times that of powder TiO2, and also has high pore volumes (0.13 cm3/g). In addition, it facilitates the separation of photogenerated carriers due to the existence of large pores that are periodically interconnected, thus, significantly improving photocatalytic efficiency. The apparent rate constant of IO TiO2 is 9.96 × 10-3 min-1, which is 1.81 times that of powder TiO2. The blue edge of 200 nm IO TiO2 is spectrally closer to the electronic band gap of TiO2. Also, it presents optimal photodegradation efficiency (70.02%), and its rate constant is 2.13 times higher than porous block TiO2 without a band gap. Moreover, a detailed path of a possible reaction mechanism is proposed based on the results of the free radical trapping experiment and EPR analysis. This research offered opportunities for a deeper understanding and more efficient utilization of the blue-edge slow light effect. The slow light can be leveraged to enhance the optical nonlinear effect, which has practical significance for solar energy collection and conversion, optical switches, and photocatalysis.
KW - band gap
KW - inverse opal TiO
KW - photocatalysis
KW - photonic nanocrystals
KW - slow light effect
UR - http://www.scopus.com/inward/record.url?scp=85197614704&partnerID=8YFLogxK
U2 - 10.1021/acsanm.4c02193
DO - 10.1021/acsanm.4c02193
M3 - Article
AN - SCOPUS:85197614704
SN - 2574-0970
VL - 7
SP - 15376
EP - 15386
JO - ACS Applied Nano Materials
JF - ACS Applied Nano Materials
IS - 13
ER -