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. 2025 Mar 5;16(1):2201.
doi: 10.1038/s41467-025-57472-8.

Perovskite spin light-emitting diodes with simultaneously high electroluminescence dissymmetry and high external quantum efficiency

Affiliations

Perovskite spin light-emitting diodes with simultaneously high electroluminescence dissymmetry and high external quantum efficiency

Shuai He et al. Nat Commun. .

Abstract

Realizing high electroluminescence dissymmetric factor and high external quantum efficiency at the same time is challenging in light-emitting diodes with direct circularly polarized emission. Here, we show that high electroluminescence dissymmetric factor and high external quantum efficiency can be simultaneously achieved in light-emitting diodes based on chiral perovskite quantum dots. Specifically, chiral perovskite quantum dots with chiral-induced spin selectivity can concurrently serve as localized radiative recombination centers of spin-polarized carriers for circularly polarized emission, thereby suppressing the relaxation of spins, Meanwhile, improving the chiral ligand exchange efficiency is found to synergistically promote their spin selectivity and optoelectronic properties so that chiroptoelectronic performance of resulting devices can be facilitated. Our device simultaneously exhibits high electroluminescence dissymmetric factor (R: 0.285 and S: 0.251) and high external quantum efficiency (R: 16.8% and S: 16%), demonstrating their potential in constructing high-performance chiral light sources.

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Conflict of interest statement

Competing interests: The authors declare no competing interests.

Figures

Fig. 1
Fig. 1. Optimization of chiroptic properties and spin selectivity in chiral PQDs for spin-LEDs.
a Schematic illustration of the mechanism of spin-LEDs based on chiral PQDs. ex: exciton, OAm: oleylamine, OAc: oleic acid. b CD and c CPL spectra of chiral CsPbBr3 PQDs with different ligand exchanged processes. US ultrasonic treatment. The corresponding d gabs and e glum values of chiral CsPbBr3 PQDs with different ligand exchange processes. f Schematic illustration of mCP-AFM measurements. Averaged I-V curves under different injected spin polarization of samples based on R-PQDs g with and h without US treatment. P: spin polarization efficiency. 30 I-V curves measured from different locations of a sample are averaged.
Fig. 2
Fig. 2. Optoelectronic properties of chiral PQDs.
a XRD, b steady-state PL and PLQY, and c TPRLspectra of chiral CsPbBr3 PQDs with and without US treatment. I-V characteristic curves of devices based on chiral PQDs d without and e with US treatments. VTFL trap-filling limit voltage. f C-ω and g Nt-Eω spectra of devices based on chiral PQDs with and without US treatment. Chiral PQDs used: R-PQDs.
Fig. 3
Fig. 3. Mechanism of the enhanced ligand exchange strategy.
TEM images of a as-synthesized achiral CsPbBr3 PQDs, b achiral CsPbBr3 PQDs without US treatment, i.e., achiral CsPbBr3 PQDs after continuous stirring, c achiral CsPbBr3 PQDs after US treatment without the addition of chiral ligands, and d chiral CsPbBr3 PQDs after ligand exchange with US treatment. Scale bar: 30 nm. Inset: corresponding HRTEM of different types of CsPbBr3 PQDs. Scale bar: 2 nm. e N 1s core level spectra and f FTIR spectra of different types of PQDs. Calculated g S(C=O)/S(-COO) and h S(C=C)/S(C-H) values obtained from FTIR spectra. i 1H-NMR spectra of chiral ligands and chiral CsPbBr3 PQDs dispersed in toluene-d8. j 1H-NMR spectra of different types of PQDs dissolved in DMSO-d6. k Calculated density density and chiral ligand exchange efficiency of different types of PQDs dissolved in DMSO-d6. Chiral PQDs used: R-PQDs.
Fig. 4
Fig. 4. Tunable chiroptic properties of chiral PQDs.
CPL spectra of a chiral CsPbCl1.5Br1.5 PQDs and b chiral CsPbI3 PQDs with R-/S-MBA. CD spectra of c chiral CsPbCl1.5Br1.5 PQDs and d chiral CsPbI3 PQDs with R-/S-MBA. CPL spectra of chiral CsPbBr3 PQDs with e R-/S-OcAm and f R-/S-AOA. CD spectra of chiral CsPbBr3 PQDs with g R-/S-OcAm and h R-/S-AOA. The above results show that the enhanced ligand exchange method is compatible with PQDs with different compositions and different types of chiral ligands.
Fig. 5
Fig. 5. Spin-LEDs based on chiral CsPbBr3 PQDs with the enhanced ligand exchange strategy.
a EL, b J-L-V, and c EQE spectra of spin-LEDs based on chiral CsPbBr3 PQDs with R- and S-MBA. Corresponding σ+ and σ emission spectra of d R-LED and e S-LED. f Wavelength-dependent gEL of R-/S-LEDs. g Summary of gEL and EQE of perovskite spin-LEDs in the literature and this work. h Time-dependent EL intensity of R-LED at an initial luminance of 100 cd m2. i T50 of R-LEDs at different initial brightness levels.

References

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