Low Lead All-Inorganic Hybrid Perovskite: A Study of Interface Defects using SCAPS-1D

Navdeep Kaur, Jaya Madan, R. Pandey
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Abstract

Hybrid perovskites are promising materials for photovoltaic applications due to their long diffusion length, high absorption coefficient, longer carrier lifetime, and adjustable bandgaps. However, the toxic nature of lead in hybrid perovskites is still a concern for the environment. In this work, a low-lead, all-inorganic perovskite material (CsP$\mathrm{b}_{0.625} Z \mathrm{n}_{0.375}$IC12) is proposed as the absorber layer. The addition of zinc reduces lead content, and all-inorganic materials have better stability against temperature and moisture variations. TiO2 is selected as the electron transport layer (ETL) and Spiro-MeOTAD as the hole transport layer (HTL) to efficiently collect the charge carriers at electrodes. The proposed design (TiO2/CsP$\mathrm{b}_{0.625} Z \mathrm{n}_{0.375}$IC1 2/SpiroMeOTAD) has been verified in the SCAPS-ID simulator under the influence of interface defect variation. Results show a decrease in current density and quantum efficiency with an increase in interface defect density at the ETL/absorber layer interface. It is observed that the current density decreases from 33.02 mA/cm2 to 29.97 mA/cm2 with an interface defect density of 1 x1010 c$\mathrm{m}^{-2}$ and 1 x101S c$\mathrm{m}^{-2}$, respectively. However, for the absorber layer/HTL interface, the current density remains constant at 33.02 mA/cm2 on variation of defect density from 1 x1010 c$\mathrm{m}^{-2}$ to 1 x101S c$\mathrm{m}^{-2}$.
低铅全无机杂化钙钛矿:用SCAPS-1D研究界面缺陷
杂化钙钛矿具有较长的扩散长度、较高的吸收系数、较长的载流子寿命和可调的带隙等优点,在光伏领域具有广阔的应用前景。然而,杂化钙钛矿中铅的毒性仍然是一个环境问题。本文提出了一种低铅全无机钙钛矿材料(CsP \ mathm {b}_{0.625} Z \ mathm {n}_{0.375}$IC12)作为吸收层。锌的加入降低了铅含量,并且全无机材料对温度和湿度变化具有更好的稳定性。选择TiO2作为电子输运层(ETL), Spiro-MeOTAD作为空穴输运层(HTL),有效地收集电极处的载流子。所提出的设计(TiO2/CsP$\ mathm {b}_{0.625} Z \ mathm {n}_{0.375}$ ic1,2 /SpiroMeOTAD)在界面缺陷变化的影响下,在SCAPS-ID模拟器上得到了验证。结果表明,随着ETL/吸收层界面缺陷密度的增加,电流密度和量子效率降低。当界面缺陷密度为1 x1010 c$\mathrm{m}^{-2}$和1 x101S c$\mathrm{m}^{-2}$时,电流密度从33.02 mA/cm2降至29.97 mA/cm2。而对于吸收层/ html界面,当缺陷密度从1 x1010 c$\ mathm {m}^{-2}$变化到1 x101S c$\ mathm {m}^{-2}$时,电流密度保持在33.02 mA/cm2不变。
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