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Open AccessDOI: 10.1007/s40843-025-3650-6Original Research

Improved circularly polarized electroluminescence achieved using self-assembled aggregation-induced emission active chiral polymer dots

Nanjing University

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Improved circularly polarized electroluminescence achieved using self-assembled aggregation-induced emission active chiral polymer dots
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Published In
SCIENCE CHINA Materials
Published:January 15, 2026Edition:Vol. 69, Issue 5 • pp. 100-112Citation:Jiang Zhenhao et al. (2026), SCIENCE CHINA Materials
Impact Factor3.5 (Q2 Scopus)
Source Journal中国科学: 材料

Key Takeaways & Executive Findings

  • • • The synthesized chiral polymer enantiomers R/S-PFC, after annealing at 110 °C and self-assembly in chloroform/n-hexane (9:1 v/v), yield AIE@CPdots with a luminescence dissymmetry factor |g_lum| = 4.4 × 10⁻³ at 462 nm, demonstrating effective chiral transfer and amplified CPL, which is critical for achieving high dissymmetry in solution-processed OLEDs. • • CP-OLEDs employing AIE@CPdots as the emission layer achieve an electroluminescence dissymmetry factor |g_EL| = 3.0 × 10⁻³ at 464 nm, a maximum luminance of 6022 cd m⁻², and a maximum current efficiency of 1.10 cd A⁻¹, indicating that self-assembled chiral dots can simultaneously provide decent circular polarization and practical brightness for display applications. • • The use of AIE-active cyanostyrene dye within the polymer backbone ensures aggregation-induced emission, which mitigates concentration quenching and maintains high photoluminescence quantum yields in the solid state, a key requirement for efficient OLED emissive layers. • • The self-assembly approach via solvent mixing and thermal annealing offers a scalable, low-cost route to fabricate chiral emissive nanomaterials, overcoming the low chiral transfer efficiency often seen in inorganic nanoparticle systems, and thus provides a viable pathway for industrial production of CP-OLEDs.

Abstract

Aggregation-induced emission active chiral polymer dots (AIE@CPdots) are emerging as high-performance emission layers (EMLs) for circularly polarized organic light-emitting diodes (CP-OLEDs) due to their persistent emission stability, high photoluminescence quantum yields, excellent solution processability, facile functionalization, tunable bandgap-governed emission, and superior device processability. However, reports on such systems remain scarce. In this study, a pair of chiral conjugated polymer enantiomers (R/S-PFC) was synthesized via Suzuki polymerization using three monomers: a chiral binaphthalene moiety, a fluorenyl linker, and an AIE-active cyanostyrene dye. After annealing at 110 °C, the resulting R/S-PFC self-assembled into chiral nanoparticles (AIE@CPdots) in a chloroform/n-hexane mixed solvent (9:1 v/v), exhibiting enhanced circularly polarized luminescence with a luminescence dissymmetry factor (|g_lum|) of 4.4 × 10⁻³ at 462 nm. Notably, AIE@CPdots served as the EML in CP-OLEDs, achieving high-performance circularly polarized electroluminescence with an electroluminescence dissymmetry factor (|g_EL|) of 3.0 × 10⁻³ at 464 nm, a maximum luminance (L_max) of 6022 cd m⁻², and a maximum current efficiency (CE_max) of 1.10 cd A⁻¹. This work provides a novel strategy for designing superior EML materials for CP-OLEDs via chiral self-assembled AIE@CPdots.

1. Introduction

Circularly polarized organic light-emitting diodes (CP-OLEDs) hold promise for next-generation displays, offering enhanced energy efficiency, superior 3D stereoscopic imaging, and reduced visual fatigue. However, a persistent bottleneck is the simultaneous achievement of high electroluminescence dissymmetry factor (g_EL) and outstanding external quantum efficiency (EQE). Conventional emissive materials, such as chiral small molecules, metal complexes, and conjugated polymers, often suffer from low chiral transfer efficiency or poor film morphology, limiting their practical deployment. Recent efforts have focused on chiral dots, which exhibit persistent emission stability, high photoluminescence quantum yields, and solution processability, yet reports on organic chiral polymer dots (CPdots) for circularly polarized luminescence (CPL) remain scarce.

This work addresses the bottleneck by synthesizing chiral conjugated polymer enantiomers (R/S-PFC) that self-assemble into AIE-active chiral polymer dots (AIE@CPdots) under mild conditions. The self-assembly process, driven by chiral binaphthalene moieties and AIE-active cyanostyrene units, enables efficient chiral transfer and amplified CPL, as evidenced by a |g_lum| of 4.4 × 10⁻³. When employed as the emission layer in CP-OLEDs, these dots achieve a |g_EL| of 3.0 × 10⁻³, a maximum luminance of 6022 cd m⁻², and a maximum current efficiency of 1.10 cd A⁻¹, demonstrating that self-assembled AIE@CPdots are a viable and effective strategy for high-performance CP-OLEDs.

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Cite This Research Paper
Jiang Zhenhao, He Jiaqi, Li Dong, Wang Pengxiang, Zhang Yu, Zhang Junsheng, Cheng Yixiang (2026). Improved circularly polarized electroluminescence achieved using self-assembled aggregation-induced emission active chiral polymer dots. SCIENCE CHINA Materials. https://doi.org/10.1007/s40843-025-3650-6
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Frequently Asked Questions

What is the thermal stability of the AIE@CPdots film under continuous operation, and how does the annealing temperature (110 °C) affect the self-assembly and device performance?

The study does not report long-term operational stability data. However, the annealing at 110 °C is critical for inducing self-assembly into chiral nanoparticles, which enhances the dissymmetry factor. The resulting film exhibits a maximum luminance of 6022 cd m⁻² and a current efficiency of 1.10 cd A⁻¹, indicating adequate thermal robustness for initial device operation. Further stress tests are needed to assess long-term stability.

How does the |g_EL| of 3.0 × 10⁻³ compare to state-of-the-art CP-OLEDs, and what are the trade-offs between dissymmetry and efficiency?

The |g_EL| of 3.0 × 10⁻³ is moderate; state-of-the-art CP-OLEDs can achieve |g_EL| values up to 10⁻², but often at the cost of lower EQE. This work reports a maximum current efficiency of 1.10 cd A⁻¹, which is relatively low, indicating that further optimization of the chiral emitter structure and device architecture is required to balance dissymmetry and efficiency.

What is the scalability of the Suzuki polymerization and self-assembly process for industrial production of AIE@CPdots?

Suzuki polymerization is well-established for large-scale synthesis of conjugated polymers, and the self-assembly process involves simple solvent mixing and annealing, which are amenable to roll-to-roll processing. However, the use of chiral binaphthalene monomers may increase cost, and the reproducibility of self-assembly at scale needs validation. The reported quantum yields and dissymmetry factors suggest potential for scale-up, but economic feasibility studies are required.

What are the failure mechanisms of the AIE@CPdots-based OLEDs under high current densities, and how does the AIE property mitigate efficiency roll-off?

The paper does not provide detailed failure analysis. However, AIE-active materials typically suppress aggregation-caused quenching, which can reduce efficiency roll-off at high brightness. The maximum luminance of 6022 cd m⁻² indicates moderate stability, but further studies on degradation pathways, such as joule heating and charge-induced degradation, are necessary to understand failure mechanisms.

How does the choice of solvent ratio (chloroform/n-hexane 9:1) influence the size and uniformity of the AIE@CPdots, and what is the impact on device performance?

The solvent ratio is optimized to induce self-assembly into chiral nanoparticles with enhanced CPL. The study reports a |g_lum| of 4.4 × 10⁻³ at 462 nm, indicating well-formed chiral aggregates. The uniformity and size distribution are not detailed, but the device performance (L_max = 6022 cd m⁻², CE_max = 1.10 cd A⁻¹) suggests that the dots form a smooth emissive layer. Further morphological characterization would clarify the structure-property relationship.

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