2020
DOI: 10.1002/anie.202006990
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Three‐Dimensional Cuprous Lead Bromide Framework with Highly Efficient and Stable Blue Photoluminescence Emission

Abstract: Considering the instability and low photoluminescence quantum yield (PLQY) of blue‐emitting perovskites, it is still challenging and attractive to construct single crystalline hybrid lead halides with highly stable and efficient blue light emission. Herein, by rationally introducing d10 transition metal into single lead halide as new structural building unit and optical emitting center, we prepared a bimetallic halide of [(NH4)2]CuPbBr5 with new type of three‐dimensional (3D) anionic framework. [(NH4)2]CuPbBr5… Show more

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Cited by 62 publications
(32 citation statements)
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“…Figure S6. The decay lifetime curves of (TPA) 2 PbBr 4 SCs at 98 K. References [3,[15][16][17][51][52][53][54][55][56][57][58][59][60] were cited in Supplementary Materials.…”
Section: Supplementary Materialsmentioning
confidence: 99%
“…Figure S6. The decay lifetime curves of (TPA) 2 PbBr 4 SCs at 98 K. References [3,[15][16][17][51][52][53][54][55][56][57][58][59][60] were cited in Supplementary Materials.…”
Section: Supplementary Materialsmentioning
confidence: 99%
“…Compared with high energy emission, low energy emission has lower activation energy resulting in the significant decreases of low band emission at high temperature (Figure S6). The low energy broadband emission at low temperature is possibly from the self‐trapped state, which is also observed in some lead halides [2d] . In addition, the maximum emission wavelength exhibits a slight red shift from 520 to 530 nm in the cooling process, which originates from the thermal expansion interaction (Figure S7).…”
Section: Resultsmentioning
confidence: 62%
“…This result indicates that at higher temperatures, more photons are coupled with excitons, thus activating the nonradiative recombination process. [ 31 ] Figure 4b exhibits the plots of integrated PL emission intensity versus the reciprocal of temperature. The activation energy ( E a ) can be derived from Arrhenius equation as follows.I(T) = I0/[ 1 + Aexp(Enormala/knormalBT) ]where I ( T ) is the emission intensity at different temperatures ( T ), and I 0 is that at 0 K, respectively.…”
Section: Resultsmentioning
confidence: 99%