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Numerical Investigation of Photo-Generated Carrier Recombination Dynamics on the Device Characteristics for the Perovskite/Carbon Nitride Absorber-Layer Solar Cell

Faisal SaeedDepartment of Electrical Engineering, Lahore University of Management Sciences (LUMS), Lahore 54792, PakistanMuhammad Haseeb KhanDepartment of Electrical Engineering, Lahore University of Management Sciences (LUMS), Lahore 54792, PakistanHaider Ali TauqeerDepartment of Electrical Engineering, Lahore University of Management Sciences (LUMS), Lahore 54792, PakistanAsfand HaroonDepartment of Electrical Engineering, University of Engineering and Technology Lahore, Lahore 39161, PakistanAsad IdreesDepartment of Electrical Engineering, Lahore University of Management Sciences (LUMS), Lahore 54792, PakistanSyed Mzhar ShehraziDepartment of Electrical Engineering, University of Lahore, Lahore 54590, PakistanLukáš ProkopENET Centre, VSB—Technical University of Ostrava, 708 00 Ostrava, Czech RepublicVojtěch BlažekENET Centre, VSB—Technical University of Ostrava, 708 00 Ostrava, Czech RepublicStanislav MišákENET Centre, VSB—Technical University of Ostrava, 708 00 Ostrava, Czech RepublicNasim UllahDepartment of Electrical Engineering, College of Engineering, Taif University, P.O. Box 11099, Taif 21944, Saudi Arabia
2022en
ABI

Аннотация

The nitrogenated holey two-dimensional carbon nitride (C2N) has been efficaciously utilized in the fabrication of transistors, sensors, and batteries in recent years, but lacks application in the photovoltaic industry. The C2N possesses favorable optoelectronic properties. To investigate its potential feasibility for solar cells (as either an absorber layer/interface layer), we foremost detailed the numerical modeling of the double-absorber-layer−methyl ammonium lead iodide (CH3NH3PbI3) −carbon nitride (C2N) layer solar cell and subsequently provided in-depth insight into the active-layer-associated recombination losses limiting the efficiency (η) of the solar cell. Under the recombination kinetics phenomena, we explored the influence of radiative recombination, Auger recombination, Shockley Read Hall recombination, the energy distribution of defects, Band Tail recombination (Hoping Model), Gaussian distribution, and metastable defect states, including single-donor (0/+), single-acceptor (−/0), double-donor (0/+/2+), double-acceptor (2/−/0−), and the interface-layer defects on the output characteristics of the solar cell. Setting the defect (or trap) density to 1015cm−3 with a uniform energy distribution of defects for all layers, we achieved an η of 24.16%. A considerable enhancement in power-conversion efficiency ( η~27%) was perceived as we reduced the trap density to 1014cm−3 for the absorber layers. Furthermore, it was observed that, for the absorber layer with double-donor defect states, the active layer should be carefully synthesized to reduce crystal-order defects to keep the total defect density as low as 1017cm−3 to achieve efficient device characteristics.

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