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基于缺陷态钝化的高效稳定蓝光钙钛矿发光二极管

吴海妍 唐建新 李艳青

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基于缺陷态钝化的高效稳定蓝光钙钛矿发光二极管

吴海妍, 唐建新, 李艳青

Efficient and stable blue perovskite light emitting diodes based on defect passivation

Wu Hai-Yan, Tang Jian-Xin, Li Yan-Qing
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  • 钙钛矿材料由于具备带隙易调、光致发光量子产率高、色纯度高、载流子迁移率高、可低温溶液加工、电荷传输性能优良等优点, 在照明显示领域大放异彩. 近年来, 通过控制化学计量比、尺寸工程和钝化缺陷等多种策略对钙钛矿微观结构进行调控, 极大地提高了钙钛矿发光二极管(perovskite light emitting diodes, PeLEDs)的性能. 目前,除蓝光外, 绿光、红光、近红外PeLEDs的外量子效率(EQE)均已超过20%. 造成蓝光器件性能停滞不前的主要原因是蓝光钙钛矿薄膜较差的覆盖率以及光谱不稳定. 为提高钙钛矿薄膜质量及器件性能, 本文在准二维钙钛矿材料PEAxCsPbBr3–yCly的基础上, 通过引入双添加剂聚乙二醇(PEG)和溴化钾(KBr), 钝化薄膜表面缺陷态, 减小晶粒尺寸, 抑制离子迁移与非辐射复合损耗, 进而提升蓝光钙钛矿器件的效率及光谱稳定性. 最终在488 nm处获得最大亮度为1049 cd·m–2, 电流效率为5.68 cd·A–1, 外量子效率为4.6%的蓝光PeLEDs. 相比于不含添加剂的器件, 效率提升了近3倍, 且具有良好的光谱稳定性和工作寿命.
    Solution-processable metal halide perovskites materials have many advantages, such as adjustable band gap, high photoluminescence quantum yield (PLQY), high color purity, high carrier mobility, low temperature solution process, excellent charge transport property and so on. These make them potential application in the display field. In the past few years, the device performance of perovskite light emitting devices (PeLEDs) have been greatly improved by manipulating the perovskite microstructures through various strategies, such as stoichiometry control, dimensional engineering, defect passivation and so on. At present, except for blue PeLEDs, the external quantum efficiencies (EQEs) over 20% have been achieved for green, red, and near-infrared PeLEDs. The low efficiency of blue PeLEDs is retarding their potential applications in full-color display and solid-state lighting. The main reasons in blue PeLEDs are the poor film coverage of blue perovskite materials and the spectral instability during device operation. In order to improve the quality of perovskite film and device performance, the quasi two-dimensional perovskite materials phenylethylammonium cesium lead bromide chloride (PEAxCsPbBr3–yCly) are used as the main perovskite emission material, by partially replacing Br with Cl to enlarge their bandgap to achieve the blue emission. The Lewis base polyethyleneglycol (PEG) is introduced to passivate the surface trapping defects and improve perovskite film coverage. The potassium bromide (KBr) is introduced to reduce perovskite grain size, suppress mobile ion migration and exhibit excellent spectral stability. Dual additives PEG and KBr are incorporated into the quasi-2D blue perovskite for inhibiting the nonradiative losses by passivating the traps in the perovskite films. Eventually, the PEAxCsPbBr3–yCly + PEG + KBr based blue PeLEDs with the emission peak of 488 nm are accompanied, which maximum brightness, current efficiency, and external quantum efficiency reached 1049 cd·m–2, of 5.68 cd·A–1, and of 4.6%, respectively, with high color purity (the Commission Internationale de L'Eclairage (CIE) chromaticity coordinates is (0.0747, 0.2570)) and the narrow full width at half maximum (FWHM) of 20 nm. Compare to the devices without additives, the efficiency has increased by nearly 3 times. Furthermore, the devices also show better spectral stability and operation lifetime. This work provides an effective method of blue PeLEDs toward the practical applications.
      通信作者: 李艳青, yqli@phy.ecnu.edu.cn
      Corresponding author: Li Yan-Qing, yqli@phy.ecnu.edu.cn
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  • 图 1  基于PEAxCsPbBr3–yCly + PEG + KBr钙钛矿前驱体溶液的合成路线

    Fig. 1.  Synthesis of PEAxCsPbBr3–yCly + PEG + KBr based perovskite precursor solution

    图 2  含有不同添加剂的PEAxCsPbBr3-yCly钙钛矿薄膜SEM图像, 标尺为200 nm

    Fig. 2.  SEM images of PEAxCsPbBr3-yCly perovskite films with different additives, the scale bar is 200 nm

    图 3  含有不同添加剂的PEAxCsPbBr3-yCly钙钛矿晶粒尺寸分布柱状图

    Fig. 3.  Histograms of grain size distributions of PEAxCsPbBr3-yCly perovskite films with different additives.

    图 4  含有不同添加剂的PEAxCsPbBr3-yCly钙钛矿薄膜在PEDOT:PSS上的XRD图谱

    Fig. 4.  XRD patterns of various PEAxCsPbBr3-yCly perovskite films with different additives on PEDOT:PSS.

    图 5  含有不同添加剂的PEAxCsPbBr3–yCly钙钛矿薄膜的光学性能表征 (a) PL光谱; (b) PLQY; (c)TRPL曲线

    Fig. 5.  Optical characterization of PEAxCsPbBr3–yCly perovskite films with different additives: (a) PL spectroscopy; (b) PLQY; (b) TRPL decay curves.

    图 6  (a) PeLEDs的器件结构示意图; (b) PeLEDs的截面SEM图像

    Fig. 6.  (a) Device structure diagram of PeLEDs; (b) Cross-sectional SEM images of PeLEDs

    图 7  含有不同添加剂的PeLEDs电学性能表征 (a)电流密度-电压-亮度(J-V-L); (b)电流效率-电流密度-外量子效率(CE-J-EQE); (c)归一化后的EL光谱图; (d)国际照明委员会(CIE)色坐标图

    Fig. 7.  Electrical performance characteristics of PeLEDs with different additives: (a) Current density-voltage-luminance(J-V-L); (b) current efficiency-current density-external quantum efficiency(CE-J-EQE); (c) the normalized EL spectra; (d) the Commission Internationale de I’Eclairage (CIE) coordinates

    图 8  (a)含有不同添加剂的PeLEDs寿命特性图. 含有不同添加剂的PeLEDs在T0T50时对应的EL光谱 (b)标准器件; (c)有PEG; (d)有PEG与KBr

    Fig. 8.  (a) Operating lifetime characteristics of PeLEDs with different additives. The corresponding EL spectra of PeLEDs with different additives at T0 and T50: (b) Control; (c) with PEG; (d) with PEG+KBr

    图 9  PeLEDs光谱稳定性 (a)标准器件; (b)有PEG; (c)有PEG与KBr

    Fig. 9.  The spectral stability of PeLEDs: (a) Control; (b) with PEG; (c) with PEG + KBr.

    图 10  5.7 V下, PeLEDs不同工作时长的EL光谱图 (a)标准器件; (b)有PEG; (c)有PEG与KBr

    Fig. 10.  The EL spectra of PeLEDs with different working minutes at 5.7 V: (a) Control; (b) with PEG; (c) with PEG+KBr.

    表 1  含有不同添加剂钙钛矿发光层的蓝光PeLEDs性能

    Table 1.  The performance of blue PeLEDs with different additive perovskite materials.

    DevicesMax.
    L/cd·m–2
    CE/cd·A–1EQE/%EL
    peak/nm
    Control7791.621.2488
    PEG10383.693.0488
    PEG+KBr10495.684.6488
    下载: 导出CSV
  • [1]

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    [2]

    姚鑫, 丁艳丽, 张晓丹, 赵颖 2015 物理学报 64 038805Google Scholar

    Yao X, Ding Y L, Zhang X D, Zhao Y 2015 Acta Phys. Sin. 64 038805Google Scholar

    [3]

    Stranks S D, Eperon G E, Grancini G, Menelaou C, Alcocer M J, Leijtens T, Herz L M, Petrozza A, Snaith H J 2013 Science 342 341Google Scholar

    [4]

    Liu D, Kelly T L 2014 Nat. Photonics 8 133Google Scholar

    [5]

    Dong Q, Fang Y, Shao Y, Mulligan P, Qiu J, Cao L, Huang J 2015 Science 347 967Google Scholar

    [6]

    Brenner P, Stulz M, Kapp D, Abzieher T, Paetzold U W, Quintilla A, Howard I A, Kalt H, Lemmer U 2016 Appl. Phys. Lett. 109 141106Google Scholar

    [7]

    Wang Y C, Li H, Hong Y H, Hong K B, Chen F C, Hsu C H, Lee R K, Conti C, Kao T S, Lu T C 2019 ACS Nano 13 5421Google Scholar

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    Xiao Z G, Kerner R A, Zhao L F, Tran N L, Lee K M, Koh T W, Scholes G D, Rand B P 2017 Nat. Photonics 11 108Google Scholar

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    Wang N, Cheng L, Ge R, Zhang S, Miao Y, Zou W, Yi C, Sun Y, Cao Y, Yang R, Wei Y, Guo Q, Ke Y, Yu M, Jin Y, Liu Y, Ding Q, Di D, Yang L, Xing G, Tian H, Jin C, Gao F, Friend R H, Wang J, Huang W 2016 Nat. Photonics 10 699Google Scholar

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    [11]

    Turkevych I, Kazaoui S, Belich N A, Grishko A Y, Fateev S A, Petrov A A, Urano T, Aramaki S, Kosar S, Kondo M, Goodilin E A, Graetzel M, Tarasov A B 2019 Nat. Nanotechnol. 14 57Google Scholar

    [12]

    Tavakoli M M, Yadav P, Prochowicz D, Sponspeller M, Osheov A, Bulovic V, Kong J 2019 Adv. Energy Mater. 9 1803587Google Scholar

    [13]

    Tan Z K, Moghaddam R S, Lai M L, Docampo P, Higler R, Deschler F, Price M, Sadhanala A, Pazos L M, Credgington D, Hanusch F, Bein T, Snaith H J, Friend R H 2014 Nat. Nanotechnol. 9 687Google Scholar

    [14]

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    黎振超, 陈梓铭, 邹广锐兴, 叶轩立, 曹镛 2019 物理学报 68 158505Google Scholar

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    王继飞, 林东旭, 袁永波 2019 物理学报 68 158501Google Scholar

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出版历程
  • 收稿日期:  2020-04-16
  • 修回日期:  2020-05-13
  • 上网日期:  2020-05-20
  • 刊出日期:  2020-07-05

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