Yulong Liu , Wenjun Liu , Li Zeng , Hongchao Huo , Suxian Ke , Xu Fan , Ying Fu
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Photophysical studies and theoretical calculations reveal that C-PyIN possesses a unique hybridized local and charge-transfer (HLCT) state property, whereas N–PyIN displays pure local excitation (LE) state emission. Notably, non-doped OLEDs incorporating C–PyIN and N–PyIN as emissive materials exhibit electroluminescent (EL) peaks at 440 nm and 444 nm, with CIE coordinates of (0.15, 0.08) and (0.15, 0.11), narrow full width at half maximum (FWHM) of 56 and 57 nm, and impressive external quantum efficiencies (EQEs) of 8.3 % and 5.0 %, respectively. More significantly, non-doped OLEDs employing C–PyIN and N–PyIN demonstrate exceptionally low efficiency roll-offs of merely 1.5 % and 6 % at a luminance of 1000 cd m<sup>–</sup><sup>2</sup>, respectively. These findings demonstrate that C-PyIN and N-PyIN are promising deep blue light-emitting materials with excellent electroluminescence performance and stability, contributing to the advancement of efficient deep blue OLEDs.</div></div>","PeriodicalId":16414,"journal":{"name":"Journal of Molecular Structure","volume":"1351 ","pages":"Article 144202"},"PeriodicalIF":4.7000,"publicationDate":"2025-10-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Highly efficient non-doped deep blue organic light-emitting diodes based on a pyreno[4,5-d]imidazole derivative with narrowband emission and small efficiency roll-off\",\"authors\":\"Yulong Liu , Wenjun Liu , Li Zeng , Hongchao Huo , Suxian Ke , Xu Fan , Ying Fu\",\"doi\":\"10.1016/j.molstruc.2025.144202\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Based on the straightforward architecture, rapid response, and support for flexible screens, organic light-emitting diodes (OLEDs) have found extensive applications in modern lighting and display systems. 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Notably, non-doped OLEDs incorporating C–PyIN and N–PyIN as emissive materials exhibit electroluminescent (EL) peaks at 440 nm and 444 nm, with CIE coordinates of (0.15, 0.08) and (0.15, 0.11), narrow full width at half maximum (FWHM) of 56 and 57 nm, and impressive external quantum efficiencies (EQEs) of 8.3 % and 5.0 %, respectively. More significantly, non-doped OLEDs employing C–PyIN and N–PyIN demonstrate exceptionally low efficiency roll-offs of merely 1.5 % and 6 % at a luminance of 1000 cd m<sup>–</sup><sup>2</sup>, respectively. 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引用次数: 0
摘要
基于简单的架构,快速响应和对柔性屏幕的支持,有机发光二极管(oled)在现代照明和显示系统中得到了广泛的应用。随着技术的进步,oled已经从早期的荧光型发展到磷光型,并最终发展到MR-TADF和HLCT等第三代系统。然而,由于其固有的宽带隙特性,蓝色OLED材料在稳定性和效率方面继续面临挑战。在这项研究中,我们提出了两种深蓝色材料C-PyIN和N-PyIN的合理设计,通过苯桥将芘[4,5-d]咪唑(PyI)单元与萘部分连接。光物理研究和理论计算表明,C-PyIN具有独特的局部和电荷转移(HLCT)杂化态,而N-PyIN具有纯局部激发(LE)态发射。值得注意的是,采用C-PyIN和N-PyIN作为发射材料的非掺杂oled在440 nm和444 nm处表现出电致发光(EL)峰,CIE坐标分别为(0.15,0.08)和(0.15,0.11),半峰全宽窄(FWHM)为56和57 nm,外部量子效率(EQEs)分别为8.3%和5.0%。更重要的是,采用C-PyIN和N-PyIN的非掺杂oled在1000 cd m-2的亮度下分别表现出1.5%和6%的极低效率滚降。这些发现表明,C-PyIN和N-PyIN具有优异的电致发光性能和稳定性,是有前途的深蓝发光材料,有助于高效深蓝oled的发展。
Highly efficient non-doped deep blue organic light-emitting diodes based on a pyreno[4,5-d]imidazole derivative with narrowband emission and small efficiency roll-off
Based on the straightforward architecture, rapid response, and support for flexible screens, organic light-emitting diodes (OLEDs) have found extensive applications in modern lighting and display systems. With technological advancements, OLEDs have evolved from early fluorescent types to phosphorescent emitters, and eventually to third-generation systems such as MR-TADF and HLCT emitters. However, blue OLED materials continue to face challenges in stability and efficiency because of their inherently wide bandgap characteristics. In this study, we present a rational design for two deep blue materials, C–PyIN and N–PyIN, achieved by linking a pyreno[4,5-d]imidazole (PyI) unit with a naphthalene moiety via a benzene bridge. Photophysical studies and theoretical calculations reveal that C-PyIN possesses a unique hybridized local and charge-transfer (HLCT) state property, whereas N–PyIN displays pure local excitation (LE) state emission. Notably, non-doped OLEDs incorporating C–PyIN and N–PyIN as emissive materials exhibit electroluminescent (EL) peaks at 440 nm and 444 nm, with CIE coordinates of (0.15, 0.08) and (0.15, 0.11), narrow full width at half maximum (FWHM) of 56 and 57 nm, and impressive external quantum efficiencies (EQEs) of 8.3 % and 5.0 %, respectively. More significantly, non-doped OLEDs employing C–PyIN and N–PyIN demonstrate exceptionally low efficiency roll-offs of merely 1.5 % and 6 % at a luminance of 1000 cd m–2, respectively. These findings demonstrate that C-PyIN and N-PyIN are promising deep blue light-emitting materials with excellent electroluminescence performance and stability, contributing to the advancement of efficient deep blue OLEDs.
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