TY - JOUR
T1 - Photoinduced Charge Carrier Dynamics of Metal Chalcogenide Semiconductor Quantum Dot Sensitized TiO2 Film for Photovoltaic Application
AU - Padmaperuma, Safna Ravindi
AU - Liu, Maning
AU - Nakamura, Ryosuke
AU - Tachibana, Yasuhiro
PY - 2021
Y1 - 2021
N2 - Semiconductor quantum dot (QD) sensitization is one of the most attractive structures to employ QDs for photovoltaic application. The function of QD sensitized solar cells (QDSSC) is controlled by the interfacial charge transfer dynamics. Here we employ transient absorption spectroscopy (TAS) to assess charge transfer dynamics at CdS QD/TiO2 interface, and correlate their dynamics with their solar cell performance. An electron injection occurs from CdS QD conduction band to TiO2 on ultrafast time scales, and the time constant decreases from ~10 ps to 1 ps, as the QD size decreases from 4 nm to 1.6 nm. Also, the charge recombination lifetime at the QD/TiO2 interface increases, as the QD size increases. An absorbed photon to current conversion efficiency (APCE) of the QDSSC increases, as the QD size increases. Therefore, we conclude that the APCE of the CdS QDSSC is controlled by the interfacial charge recombination dynamics competing with dynamics of the hole transfer from the QD valence band to the reduced electrolyte. The optimum CdS QD size is close to or larger than 4 nm, as long as the light harvesting efficiency of the CdS QD sensitized film is sufficiently high.
AB - Semiconductor quantum dot (QD) sensitization is one of the most attractive structures to employ QDs for photovoltaic application. The function of QD sensitized solar cells (QDSSC) is controlled by the interfacial charge transfer dynamics. Here we employ transient absorption spectroscopy (TAS) to assess charge transfer dynamics at CdS QD/TiO2 interface, and correlate their dynamics with their solar cell performance. An electron injection occurs from CdS QD conduction band to TiO2 on ultrafast time scales, and the time constant decreases from ~10 ps to 1 ps, as the QD size decreases from 4 nm to 1.6 nm. Also, the charge recombination lifetime at the QD/TiO2 interface increases, as the QD size increases. An absorbed photon to current conversion efficiency (APCE) of the QDSSC increases, as the QD size increases. Therefore, we conclude that the APCE of the CdS QDSSC is controlled by the interfacial charge recombination dynamics competing with dynamics of the hole transfer from the QD valence band to the reduced electrolyte. The optimum CdS QD size is close to or larger than 4 nm, as long as the light harvesting efficiency of the CdS QD sensitized film is sufficiently high.
KW - CdS quantum dot sensitized TiO
KW - Charge recombination
KW - Electron injection
KW - Photocurrent generation efficiency
KW - Quantum dot size
KW - Solar cells
U2 - 10.2494/PHOTOPOLYMER.34.271
DO - 10.2494/PHOTOPOLYMER.34.271
M3 - Article
AN - SCOPUS:85123783388
SN - 0914-9244
VL - 34
SP - 271
EP - 278
JO - Journal of Photopolymer Science and Technology
JF - Journal of Photopolymer Science and Technology
IS - 3
ER -