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Phase Segregation in Potassium-Doped Lead Halide Perovskites from ~(39)K Solid-State NMR at 21.1 T

机译:〜(39)K固态NMR在21.1 T下掺杂钾的卤化铅钙钛矿中的相分离

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摘要

Organic–inorganic lead halide perovskites are a promising family of light absorbers for a new generation of solar cells, with reported efficiencies currently exceeding 22%. A common problem of solar cells fabricated using these materials is that their efficiency depends on their cycling history, an effect known as current–voltage (J –V ) hysteresis. Potassium doping has recently emerged as a universal way to overcome this adverse phenomenon. While the atomistic origins of J –V hysteresis are still not fully understood, it is essential to rationalize the atomic-level effect of protocols that lead to its suppression. Here, using ~(39)K MAS NMR at 21.1 T we provide for the first time atomic-level characterization of the potassium-containing phases that are formed upon KI doping of multication and multianion lead halide perovskites. We find no evidence of potassium incorporation into 3D perovskite lattices of the recently reported materials. Instead, we observe formation of a mixture of potassium-rich phases and unreacted KI. In the case of Br-containing lead halide perovskites doped with KI, a mixture of KI and KBr ensues, leading to a change in the Br/I ratio in the perovskite phase with respect to the undoped perovskite. Simultaneous Cs and K doping leads to the formation of nonperovskite Cs/K lead iodide phases.
机译:有机-无机卤化铅钙钛矿是用于新一代太阳能电池的有前途的光吸收剂系列,目前报道的效率超过22%。使用这些材料制造的太阳能电池的一个普遍问题是其效率取决于其循环历史,这种效应被称为电流-电压(iJ–iV)滞后现象。钾掺杂最近已成为克服这种不利现象的通用方法。尽管仍未完全了解J i –V V磁滞的原子起源,但合理化导致其抑制的协议的原子级影响是至关重要的。在这里,我们使用21.1 T处的〜(39)K MAS NMR,首次提供了对多阳离子和多阴离子卤化铅钙钛矿进行KI掺杂后形成的含钾相的原子级表征。我们没有发现钾结合到最近报道的材料的3D钙钛矿晶格中的证据。相反,我们观察到形成了富钾相和未反应的KI的混合物。在掺有KI的含Br的卤化铅钙钛矿中,随之而来的是KI和KBr的混合物,导致钙钛矿相相对于未掺杂的钙钛矿的Br / I比发生变化。同时掺杂Cs和K导致形成非钙钛矿Cs / K碘化铅相。

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  • 来源
    《Journal of the American Chemical Society》 |2018年第23期|7232-7238|共7页
  • 作者单位

    Laboratory of Magnetic Resonance, Institute of Chemical Sciences and Engineering and Laboratory of Photonics and Interfaces, Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland;

    Laboratory of Magnetic Resonance, Institute of Chemical Sciences and Engineering and Laboratory of Photonics and Interfaces, Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland,Institute of Physical Chemistry, Polish Academy of Sciences, Kasprzaka 44/52, 01-224 Warsaw, Poland;

    Laboratory of Magnetic Resonance, Institute of Chemical Sciences and Engineering and Laboratory of Photonics and Interfaces, Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland;

    Laboratory of Magnetic Resonance, Institute of Chemical Sciences and Engineering and Laboratory of Photonics and Interfaces, Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland;

    Laboratory of Magnetic Resonance, Institute of Chemical Sciences and Engineering and Laboratory of Photonics and Interfaces, Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland;

    Laboratory of Magnetic Resonance, Institute of Chemical Sciences and Engineering and Laboratory of Photonics and Interfaces, Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland;

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  • 正文语种 eng
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  • 入库时间 2022-08-18 03:07:21

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