Correction to “Efficient Interfacial Upconversion Enabling Bright Emission at an Extremely Low Driving Voltage in Organic Light-Emitting Diodes”

IF 7.2 2区 材料科学 Q1 MATERIALS SCIENCE, MULTIDISCIPLINARY
Advanced Optical Materials Pub Date : 2026-04-05 Epub Date: 2026-03-19 DOI:10.1002/adom.71111
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However, the actual wavelength interval of the acquired spectral data was 0.57–0.60 nm. After re-evaluating the calculation using this data interval as the wavelength interval, we found that the corrected values are approximately three-sevenths of those reported previously. 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All relative comparisons between materials and experimental conditions remain unchanged, as they are scaled uniformly. The corrected maximum efficiency of our upconversion (UC)-organic light-emitting diode (OLED) is 1.20%, which is two orders of magnitude higher than that in the previous UC-OLED (0.043%). This correction does not affect the main claim of the original paper, two orders of magnitude higher EQE and bright UC emission at a low voltage.</p><p>In addition, the authors would like to correct <i>Φ</i><sub>PL</sub>: absolute photoluminescence quantum efficiency (PLQE) values of pristine rubrene and rubrene doped with 0.5 vol% DBP films in Table S1. The reevaluated PLQE of the pristine rubrene film is 2.8% (29.1% in the original paper), and that of the rubrene doped with 0.5 vol% DBP film is 44.9% (72.6% in the original paper). In the previous experiment, the rubrene films were encapsulated, and the epoxy resin, applied to the edge of the substrate, swelled the rubrene, making it emissive. The swelled edge part was excited in an integrating sphere for PLQE measurement and contributed to additional emission. The corrected data were measured on the film without encapsulation. The authors are therefore replacing the original Table S1 with the new Table S1 in the latest version of the Supporting Information.</p><p>To compare the PL intensity of different doping concentrations of DBP, the authors are adding normalized PL spectra of pristine and DBP-doped rubrene films at 500 nm as Figure S2b in the latest version of the Supporting Information, in addition to the original Figure S2 of PL spectra normalized at the maximum peak intensity. 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引用次数: 0

Abstract

S. Izawa, M. Morimoto, S. Naka, et al.: Efficient Interfacial Upconversion Enabling Bright Emission at an Extremely Low Driving Voltage in Organic Light-Emitting Diodes. Adv. Optical Mater. 10, 2101710 (2022). https://doi.org/10.1002/adom.202101710.

In the above article, the authors would like to correct an error identified in the calculation of the external quantum efficiency (EQE). Specifically, the error originates from the choice of wavelength interval (nm) used in the numerical integration of spectral data. In the original manuscript, the wavelength interval was taken to be 1.4 nm, corresponding to the stated instrumental spectral resolution of the spectrometer. However, the actual wavelength interval of the acquired spectral data was 0.57–0.60 nm. After re-evaluating the calculation using this data interval as the wavelength interval, we found that the corrected values are approximately three-sevenths of those reported previously. The corrected calculation procedure was quantitatively validated by comparison with independently calibrated measurements obtained using an EQE measurement system based on an integrating sphere.

The authors are therefore replacing the original Figures 3 and S6 with the new Figures 3 and S6 below, which are based on the verified procedure.

FIGURE 3 | EQE as a function of injected current density for (a) rubrene/C60 (black circle), rubrene/C8-PTCDI (red triangle), DBP-doped rubrene/C60 (blue cross), and DBP-doped rubrene/C8-PTCDI (purple square) devices with an emitter layer thickness of 50 nm; and (b) DBP-doped rubrene/C8-PTCDI devices with different emitter layer thicknesses, i.e., 20 nm (gray diamond), 50 nm (purple square), 100 nm (blue triangle), 150 nm (orange cross), and 200 nm (green circle).

The corrected Figure S6 is listed in the latest version of the Supporting Information.

It is important to note that this correction only applies to the absolute values. All relative comparisons between materials and experimental conditions remain unchanged, as they are scaled uniformly. The corrected maximum efficiency of our upconversion (UC)-organic light-emitting diode (OLED) is 1.20%, which is two orders of magnitude higher than that in the previous UC-OLED (0.043%). This correction does not affect the main claim of the original paper, two orders of magnitude higher EQE and bright UC emission at a low voltage.

In addition, the authors would like to correct ΦPL: absolute photoluminescence quantum efficiency (PLQE) values of pristine rubrene and rubrene doped with 0.5 vol% DBP films in Table S1. The reevaluated PLQE of the pristine rubrene film is 2.8% (29.1% in the original paper), and that of the rubrene doped with 0.5 vol% DBP film is 44.9% (72.6% in the original paper). In the previous experiment, the rubrene films were encapsulated, and the epoxy resin, applied to the edge of the substrate, swelled the rubrene, making it emissive. The swelled edge part was excited in an integrating sphere for PLQE measurement and contributed to additional emission. The corrected data were measured on the film without encapsulation. The authors are therefore replacing the original Table S1 with the new Table S1 in the latest version of the Supporting Information.

To compare the PL intensity of different doping concentrations of DBP, the authors are adding normalized PL spectra of pristine and DBP-doped rubrene films at 500 nm as Figure S2b in the latest version of the Supporting Information, in addition to the original Figure S2 of PL spectra normalized at the maximum peak intensity. The peak intensity reaches its maximum at the 0.5% doping concentration primarily used in the OLED devices in this paper.

Based on the corrected EQEMax and ΦPL, the authors recalculated ΦLoss and are therefore replacing the original Table 2 with the new Table 2 below.

Additionally, the authors would like to correct an error in the unit of luminance. The labeled “cd/cm2” in Figure 2b,d, and Figures S3, S5, and S7 in the Supporting Information were incorrect. These should be corrected to “cd/m2”.

FIGURE 2 | (a) J–V and (b) L–V curves for rubrene/BCP control (gray diamond), rubrene/C60 (black circle), rubrene/C8-PTCDI (red triangle), DBP-doped rubrene/C8-PTCDI (green cross) without a rubrene interlayer, and DBP-doped rubrene/C8-PTCDI (purple square) devices. (c) EL emission spectra of rubrene/C8-PTCDI (red) and DBP-doped rubrene/C8-PTCDI (purple) devices under a constant applied current (123 mA/cm2). (d) J–V and corrected L–V curves of rubrene/C8-PTCDI (red triangle) and DBP-doped rubrene/C8-PTCDI (purple square) devices measured using a photodetector. The EL intensity was corrected to correspond with that measured using the luminance meter in b. (e) Photograph of a DBP-doped rubrene/C8-PTCDI device operated by a 1.5-V battery.

The corrected Figures S3, S5, and S7 are listed in the latest version of the Supporting Information.

The authors apologize for any confusion this may have caused and state that the scientific conclusions of the original article are unaffected.

修正“有机发光二极管在极低驱动电压下实现明亮发射的高效界面上转换”
S. Izawa, M. Morimoto, S. Naka等:在极低驱动电压下实现有机发光二极管亮发射的高效界面上转换。光学材料学报,2017,21(2):481 - 481。https://doi.org/10.1002/adom.202101710.In在上述文章中,作者想纠正在计算外部量子效率(EQE)时发现的一个错误。具体来说,误差来源于光谱数据数值积分中波长间隔(nm)的选择。在原稿中,取波长间隔为1.4 nm,对应于所述光谱仪的仪器光谱分辨率。而实际获得的光谱数据波长间隔为0.57 ~ 0.60 nm。在使用该数据间隔作为波长间隔重新评估计算后,我们发现校正值约为先前报告值的七分之三。通过与基于积分球的EQE测量系统独立标定的测量结果进行比较,对修正后的计算方法进行了定量验证。因此,作者将原来的图3和S6替换为下面基于验证程序的新图3和S6。图3 (a)发射极层厚度为50 nm的rubrene/C60(黑圈)、rubrene/C8-PTCDI(红三角)、dbp掺杂rubrene/C60(蓝十字)和dbp掺杂rubrene/C8-PTCDI(紫方)器件的| EQE与注入电流密度的关系;(b)不同发射层厚度的dbp掺杂rubrene/C8-PTCDI器件,分别为20 nm(灰色菱形)、50 nm(紫色方形)、100 nm(蓝色三角形)、150 nm(橙色十字)和200 nm(绿色圆圈)。更正后的图S6载于最新版本的“支持资料”内。重要的是要注意,这种修正只适用于绝对值。材料和实验条件之间的所有相对比较都保持不变,因为它们是均匀缩放的。我们的上转换(UC)有机发光二极管(OLED)的修正最大效率为1.20%,比之前的UC-OLED(0.043%)提高了两个数量级。这一修正并不影响原论文的主要主张,在低电压下,EQE和明亮的UC发射提高了两个数量级。此外,作者想要更正ΦPL:表S1中原始rubrene和掺杂0.5 vol% DBP薄膜的rubrene的绝对光致发光量子效率(PLQE)值。原始rubrene薄膜重估PLQE为2.8%(原论文为29.1%),掺杂0.5 vol% DBP薄膜的rubrene重估PLQE为44.9%(原论文为72.6%)。在之前的实验中,将rubrene薄膜封装,并将环氧树脂涂在基材边缘,使rubrene膨胀,使其发光。在PLQE测量中,膨胀边缘部分在积分球中被激发,并对附加发射有贡献。校正后的数据在未封装的薄膜上测量。因此,作者在最新版本的支持信息中用新的表S1取代了原来的表S1。为了比较不同掺杂浓度DBP的发光强度,作者在原有的最大峰强度归一化发光光谱图S2之外,在最新版本的support Information中增加了原始和掺DBP的rubrene薄膜在500 nm处的归一化发光光谱,如图S2b所示。在本文中主要用于OLED器件的掺杂浓度为0.5%时,峰值强度达到最大。根据修正后的EQEMax和ΦPL,作者重新计算了ΦLoss,因此用下面的新表2取代了原来的表2。此外,作者希望纠正亮度单位中的一个错误。“支持信息”中图2b、d和图S3、S5、S7标注的“cd/cm2”不正确。这些应该更正为“cd/m2”。图2 | (a) J-V和(b) L-V曲线为rubrene/BCP对照(灰色菱形)、rubrene/C60(黑色圆圈)、rubrene/C8-PTCDI(红色三角形)、不含rubrene中间层的dbp掺杂rubrene/C8-PTCDI(绿色十字)和dbp掺杂rubrene/C8-PTCDI(紫色方框)器件。(c)恒定电流(123 mA/cm2)下rubrene/C8-PTCDI(红色)和dbp掺杂rubrene/C8-PTCDI(紫色)器件的EL发射光谱。(d)利用光电探测器测量rubrene/C8-PTCDI(红色三角形)和dbp掺杂rubrene/C8-PTCDI(紫色方形)器件的J-V曲线和校正后的L-V曲线。对EL强度进行校正,使其与b中亮度计测量的EL强度相一致。(e)由1.5 v电池供电的掺dbp的rubrene/C8-PTCDI器件的照片。更正后的图S3、S5及S7列于最新版本的“支持资料”内。 作者为这可能造成的任何混乱表示歉意,并声明原始文章的科学结论不受影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Advanced Optical Materials
Advanced Optical Materials MATERIALS SCIENCE, MULTIDISCIPLINARY-OPTICS
CiteScore
13.70
自引率
6.70%
发文量
883
审稿时长
1.5 months
期刊介绍: Advanced Optical Materials, part of the esteemed Advanced portfolio, is a unique materials science journal concentrating on all facets of light-matter interactions. For over a decade, it has been the preferred optical materials journal for significant discoveries in photonics, plasmonics, metamaterials, and more. The Advanced portfolio from Wiley is a collection of globally respected, high-impact journals that disseminate the best science from established and emerging researchers, aiding them in fulfilling their mission and amplifying the reach of their scientific discoveries.
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