2022
DOI: 10.1021/acs.jpclett.2c01199
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Zn2+-Doped Lead-Free CsMnCl3 Nanocrystals Enable Efficient Red Emission with a High Photoluminescence Quantum Yield

Abstract: The toxicity of Pb and the instability of lead halide perovskites are the main obstacles to the practical application of lead-based nanocrystals (NCs). In this paper, all-inorganic Zn2+-doped lead-free perovskite (CsMn1–x Zn x Cl3) NCs were synthesized by a hot-injection method. Mn2+ ions were partially replaced by Zn2+ ions, and the energy transfer between Mn2+ was effectively suppressed. Because of this, excitons are more advantageously confined to the [MnCl6]4– octahedron. Target CsMn0.95Zn0.05Cl3 NCs were … Show more

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Cited by 23 publications
(49 citation statements)
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“…The binding energy of 100 meV is higher than that of 3D LHPs and comparable to those of all-inorganic 1D lead-free halide perovskites or quasi-2D organic–inorganic hybrid perovskites. A high E b value indicates strong confinement of the excitons in the r-CsMnCl 3 NCs, which might explain its high PLQY. The fwhm of the emission decreases from 69 to 52 meV when the sample cools down from 293 to 50 K (Figure S7), consistent with the earlier studies on the NCs. , The gradual drop in the fwhm of the NCs with decreasing temperature suggests reduced exciton phonon coupling strength (lattice vibrations), which contributes to the increased integrated PL intensity (Figure c). , …”
Section: Resultssupporting
confidence: 88%
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“…The binding energy of 100 meV is higher than that of 3D LHPs and comparable to those of all-inorganic 1D lead-free halide perovskites or quasi-2D organic–inorganic hybrid perovskites. A high E b value indicates strong confinement of the excitons in the r-CsMnCl 3 NCs, which might explain its high PLQY. The fwhm of the emission decreases from 69 to 52 meV when the sample cools down from 293 to 50 K (Figure S7), consistent with the earlier studies on the NCs. , The gradual drop in the fwhm of the NCs with decreasing temperature suggests reduced exciton phonon coupling strength (lattice vibrations), which contributes to the increased integrated PL intensity (Figure c). , …”
Section: Resultssupporting
confidence: 88%
“…The temperature-dependent PL quenching of the r-CsMnCl 3 NCs (100–300 K) can be expressed via the following equation I ( T ) = I 0 1 + A .25em normale E b / k B T where I ( T ) and I 0 are the PL intensities at temperatures T and 0 K, respectively, E b is the exciton binding energy, and k B is the Boltzmann constant. By fitting the PL quenching data using the above equation, an exciton binding energy ( E b ) value of 100 ± 18 meV is extracted (Figure b), which closely matches the earlier reported value (81.36 meV) . The binding energy of 100 meV is higher than that of 3D LHPs and comparable to those of all-inorganic 1D lead-free halide perovskites or quasi-2D organic–inorganic hybrid perovskites. A high E b value indicates strong confinement of the excitons in the r-CsMnCl 3 NCs, which might explain its high PLQY.…”
Section: Resultssupporting
confidence: 82%
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“…Similar to the above‐discussed CANIC matrix, partial substitution of Mn 2+ with Zn 2+ cations in the nanocrystalline CsMnCl 3 host resulted in efficient spatial confinement of MnCl 6 octahedra, thus prohibiting energy migration between Mn‐based centers and boosting STE PL QY up to ca. 77 % [42] …”
Section: Other Emerging Lfp Host Matricesmentioning
confidence: 99%
“…77 % erhöht wurde. [42] Eine starke Verzerrung des BHP-Gitters durch "fremde" Liganden kann ebenfalls zu bemerkenswerten Veränderungen der spektralen STE-PL-Parameter führen, wie für das Sb-dotierte Paar Rb 3 InCl 6 /Rb 2 InCl 5 (H 2 O) gezeigt wird. [28] Je nach der Bindung des "fremden" Liganden an die M III -Stelle kann diese Veränderung reversibel sein und eine zusätzliche Kontrolle über die PL-Farbe ermöglichen.…”
Section: Csmncl 3 -Matrixunclassified