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利用抗磁系数估计二维层状钙钛矿中的有效质量减小:来自高磁场光谱学的新见解。

Using the Diamagnetic Coefficients to Estimate the Reduced Effective Mass in 2D Layered Perovskites: New Insight from High Magnetic Field Spectroscopy.

机构信息

Department of Experimental Physics, Faculty of Fundamental Problems of Technology, Wroclaw University of Science and Technology, 50-370 Wroclaw, Poland.

出版信息

Int J Mol Sci. 2022 Oct 19;23(20):12531. doi: 10.3390/ijms232012531.

DOI:10.3390/ijms232012531
PMID:36293385
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9604088/
Abstract

In this work, the current state of research concerning the determination of the effective mass in 2D layered perovskites is presented. The available experimental reports in which the reduced effective mass μ has been directly measured using magneto-absorption spectroscopy of interband Landau levels are reviewed. By comparing these results with DFT computational studies and various other methods, it is concluded that depending on the approach used, the μ found spans a broad range of values from as low as 0.05 up to 0.3 me. To facilitate quick and reliable estimation of μ, a model is proposed based solely on the available experimental data that bypass the complexity of interband Landau level spectroscopy. The model takes advantage of the μ value measured for (PEA)2PbI4 and approximates the reduced effective mass of the given 2D layered perovskites based on only two experimental parameters-the diamagnetic coefficient and the effective dielectric constant. The proposed model is tested on a broad range of 2D layered perovskites and captures well the main experimental and theoretical trends.

摘要

在这项工作中,呈现了关于二维层状钙钛矿中有效质量确定的研究现状。综述了利用带间朗道能级的磁吸收光谱直接测量得到的有效质量μ的现有实验报告。通过将这些结果与密度泛函理论(DFT)计算研究和各种其他方法进行比较,可以得出结论,根据所采用的方法,所得到的μ值范围很广,从低至 0.05 到 0.3 me。为了便于快速可靠地估计μ,提出了一个仅基于现有实验数据的模型,该模型绕过了带间朗道能级光谱的复杂性。该模型利用(PEA)2PbI4 测量的μ值,并仅基于两个实验参数——抗磁系数和有效介电常数,来近似给定二维层状钙钛矿的有效质量。该模型在广泛的二维层状钙钛矿上进行了测试,很好地捕捉了主要的实验和理论趋势。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/9671311d024f/ijms-23-12531-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/9bb1a39c5b53/ijms-23-12531-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/b1da4fb5c6b7/ijms-23-12531-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/095a31f5c262/ijms-23-12531-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/9671311d024f/ijms-23-12531-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/9bb1a39c5b53/ijms-23-12531-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/b1da4fb5c6b7/ijms-23-12531-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/095a31f5c262/ijms-23-12531-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b0ae/9604088/9671311d024f/ijms-23-12531-g004.jpg

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