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Impact of Layer Thickness on the Charge Carrier and Spin Coherence Lifetime in Two-Dimensional Layered Perovskite Single Crystals AITranslate

National Renewable Energy Laboratory; National Renewable Energy Laboratory; National Renewable Energy Laboratory; National Renewable Energy Laboratory; National Renewable Energy Laboratory; National Renewable Energy Laboratory; National Renewable Energy Laboratory; National Renewable Energy Laboratory; National Renewable Energy Laboratory
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Publisher: ACS
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Abstract AITranslate

We report the charge carrier recombination rate and spin coherence lifetimes in single crystals of two-dimensional (2D) Ruddlesden–Popper perovskites PEA2PbI4·(MAPbI3)n−1 (PEA, phenethylammonium; MA, methylammonium; n = 1, 2, 3, 4). Layer thickness-dependent charge carrier recombination rates are observed, with the fastest rates for n = 1 because of the large exciton binding energy, and the slowest rates are observed for n = 2. Room-temperature spin coherence times also show a nonmonotonic layer thickness dependence with an increasing spin coherence lifetime with increasing layer thickness from n = 1 to n = 4, followed by a decrease in lifetime from n = 4 to ∞. The longest coherence lifetime of ∼7 ps is observed in the n = 4 sample. Our results are consistent with two contributions: Rashba splitting increases the spin coherence lifetime going from the n = ∞ to the layered systems, while phonon scattering, which increases for smaller layers, decreases the spin coherence lifetime. The interplay between these two factors contributes to the layer thickness dependence.

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DOI:https://doi.org/10.1021/acsenergylett.8b01315

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We report the charge carrier recombination rate and spin coherence lifetimes in single crystals of two-dimensional (2D) Ruddlesden–Popper perovskites PEA2PbI4·(MAPbI3)n−1 (PEA, phenethylammonium; MA, methylammonium; n = 1, 2, 3, 4). Layer thickness-dependent charge carrier recombination rates are observed, with the fastest rates for n = 1 because of the large exciton binding energy, and the slowest rates are observed for n = 2. Room-temperature spin coherence times also show a nonmonotonic layer thickness dependence with an increasing spin coherence lifetime with increasing layer thickness from n = 1 to n = 4, followed by a decrease in lifetime from n = 4 to ∞. The longest coherence lifetime of ∼7 ps is observed in the n = 4 sample. Our results are consistent with two contributions: Rashba splitting increases the spin coherence lifetime going from the n = ∞ to the layered systems, while phonon scattering, which increases for smaller layers, decreases the spin coherence lifetime. The interplay between these two factors contributes to the layer thickness dependence.

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GB/T 7714-2015 [1] Xihan Chen, Haipeng Lu, Zhen Li, et al. ACS Energy Letters, 2018(3). DOI:10.1021/acsenergylett.8b01315.
MLA [1] Xihan Chen, et al., ACS Energy Letters, no. 3, 2018, https://doi.org/10.1021/acsenergylett.8b01315.
APA [1] Xihan Chen, Haipeng Lu, Zhen Li, Yaxin Zhai, Paul F. Ndione, Joseph J. Berry, Kai Zhu, Ye Yang, & Matthew C. Beard. (2018). ACS Energy Letters(3). https://doi.org/10.1021/acsenergylett.8b01315
IEEE [1] Xihan Chen, Haipeng Lu, Zhen Li, Yaxin Zhai, Paul F. Ndione, Joseph J. Berry, Kai Zhu, Ye Yang, and Matthew C. Beard, ACS Energy Letters, no. 3, 2018, doi: 10.1021/acsenergylett.8b01315.