In the present study, we studied the capacitance frequency response of amorphous titanium dioxide (A-TiO2)/poly(3-hexylthiophene) (P3HT) solar cells. The capacitance was measured to provide information on interfacial layer between the two materials. At a low frequency, the capacitance increased because the frequency was lower than the relaxation time of the charge carriers, thus providing evidence of the formation of a depletion region at the P3HT/A-TiO2 interface. The loss tangent was measured for applied voltage ranging from 0 to 1.5 V and the frequencies from 20 Hz and 1 MHz. Peaks in the loss tangent appeared as a function of the applied voltage due to changes in the transport and accumulation mechanisms of charge at the interface and the presence of oxygen molecules in the TiO2. The resulting C-V curves were used to calculate dopant concentration and the barrier's potential, which was found to 1017 cm−3 and 0.6 V, respectively. This confirmed the presence of a depletion region placed in the P3HT region and the validated barrier's potential effect on the open circuit voltage value. It was also shown that the light J-V characteristics of the A-TiO2/P3HT solar cells were independent of the ambient conditions because the conductivity of P3HT and the depletion region were not affected.
Citation: Hmoud. Al-Dmour. Capacitance response of solar cells based on amorphous Titanium dioxide (A-TiO2) semiconducting heterojunctions[J]. AIMS Materials Science, 2021, 8(2): 261-270. doi: 10.3934/matersci.2021017
In the present study, we studied the capacitance frequency response of amorphous titanium dioxide (A-TiO2)/poly(3-hexylthiophene) (P3HT) solar cells. The capacitance was measured to provide information on interfacial layer between the two materials. At a low frequency, the capacitance increased because the frequency was lower than the relaxation time of the charge carriers, thus providing evidence of the formation of a depletion region at the P3HT/A-TiO2 interface. The loss tangent was measured for applied voltage ranging from 0 to 1.5 V and the frequencies from 20 Hz and 1 MHz. Peaks in the loss tangent appeared as a function of the applied voltage due to changes in the transport and accumulation mechanisms of charge at the interface and the presence of oxygen molecules in the TiO2. The resulting C-V curves were used to calculate dopant concentration and the barrier's potential, which was found to 1017 cm−3 and 0.6 V, respectively. This confirmed the presence of a depletion region placed in the P3HT region and the validated barrier's potential effect on the open circuit voltage value. It was also shown that the light J-V characteristics of the A-TiO2/P3HT solar cells were independent of the ambient conditions because the conductivity of P3HT and the depletion region were not affected.
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