用DLTS和DLOS表征的CZTSSe太阳能电池中的少数载流子电子陷阱

V. Kheraj, E. Lund, A. E. Caruso, K. Al-Ajmi, D. Pruzan, C. Miskin, R. Agrawal, C. Beall, I. Repins, M. Scarpulla
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引用次数: 0

摘要

本文报道了在6-8%效率的Cu2ZnSn(S, Se)4 (CZTSSe)器件中,利用传统和少数深能级瞬态光谱(dts)和深能级光学光谱(DLOS)观察到的少数载流子与深能级的相互作用。直接观察缺陷与少数载流子的相互作用是理解深层重组影响的关键。在具有Cu2ZnSn(S, Se)4纳米颗粒油墨吸收层的器件中,我们发现了捕获和发射少数电子的中隙状态。它距离导带迁移率边缘为590±50 meV,浓度接近1015/cm3,表观电子捕获截面~10-14 cm2。我们的结论是,虽然能量定位几乎是理想的重组中心,但这些缺陷由于更小的空穴横截面而充当电子陷阱。在使用共蒸发生产的CZTSe器件中,我们在传统样品以及具有透明欧姆背触点的样品上使用了少数载流子dlt。这些实验展示了明确探测太阳能电池中少数载流子/缺陷相互作用的方法,以便在缺陷能级观测和少数载流子寿命之间建立直接联系。此外,我们演示了使用稳态器件模拟来帮助解释DLTS结果,例如,即使在没有直接测量的情况下,也可以在互补载波截面上设置边界。这种结合实验和理论的方法建立了严格的限制,对载流子寿命和Voc缺陷的影响与DLTS观察到的相反,例如,假设所有深态都充当强重组中心。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Minority carrier electron traps in CZTSSe solar cells characterized by DLTS and DLOS
We report observations of minority carrier interactions with deep levels in 6-8% efficient Cu2ZnSn(S, Se)4 (CZTSSe) devices using conventional and minority deep level transient spectroscopy (DLTS) and deep level optical spectroscopy (DLOS). Directly observing defect interactions with minority carriers is critical to understanding the recombination impact of deep levels. In devices with Cu2ZnSn(S, Se)4 nanoparticle ink absorber layers we identify a mid-gap state capturing and emitting minority electrons. It is 590±50 meV from the conduction band mobility edge, has a concentration near 1015/cm3, and has an apparent electron capture cross section ~10-14 cm2. We conclude that, while energetically positioned nearly-ideally to be a recombination center, these defects instead act as electron traps because of a smaller hole cross-section. In CZTSe devices produced using coevaporation, we used minority carrier DLTS on traditional samples as well as ones with transparent Ohmic back contacts. These experiments demonstrate methods for unambiguously probing minority carrier/defect interactions in solar cells in order to establish direct links between defect energy level observations and minority carrier lifetimes. Furthermore, we demonstrate the use of steady-state device simulation to aid in the interpretation of DLTS results e.g. to put bounds on the complimentary carrier cross section even in the absence its direct measurement. This combined experimental and theoretical approach establishes rigorous bounds on the impact on carrier lifetime and Voc of defects observed with DLTS as opposed to, for example, assuming that all deep states act as strong recombination centers.
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