2018
DOI: 10.1021/acsenergylett.8b00758
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Efficient Photon Recycling and Radiation Trapping in Cesium Lead Halide Perovskite Waveguides

Abstract: Cesium lead halide perovskite materials have attracted considerable attention for potential applications in lasers, light emitting diodes and photodetectors. Here, we provide the experimental and theoretical evidence for photon recycling in CsPbBr3 perovskite microwires. Using twophoton excitation, we recorded photoluminescence (PL) lifetimes and emission spectra as a function of the lateral distance between PL excitation and collection positions along the microwire,

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Cited by 72 publications
(101 citation statements)
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“…Intriguing phenomena such as anomalous photovoltaic effect, phonon recycling, and optical cooling have been observed in halide perovskites. [ 9–12 ] For example, it was recently proposed that bright triplet excitons are behind the frequently observed high PL quantum yield in halide perovskites. [ 13 ] Halide perovskites with the general chemical formula of ABX 3 , where A is an organic or inorganic cation, B a metal cation, and X a halide anion, present unique opportunities to realize versatile material properties through manipulating the cation and halide compositions.…”
Section: Introductionmentioning
confidence: 99%
“…Intriguing phenomena such as anomalous photovoltaic effect, phonon recycling, and optical cooling have been observed in halide perovskites. [ 9–12 ] For example, it was recently proposed that bright triplet excitons are behind the frequently observed high PL quantum yield in halide perovskites. [ 13 ] Halide perovskites with the general chemical formula of ABX 3 , where A is an organic or inorganic cation, B a metal cation, and X a halide anion, present unique opportunities to realize versatile material properties through manipulating the cation and halide compositions.…”
Section: Introductionmentioning
confidence: 99%
“…These characteristics make them excellent candidates for optoelectronic applications such as lightemitting diodes [6][7] , lasers 8 , and photodetectors [9][10] . Unlike the well-studied three-dimensional (3D) perovskite structures (e.g., CsPbBr3) [11][12][13][14][15] , 0D perovskites are bulk quantum materials without corner-sharing connectivity; and as a result, their optical and photo-physical properties, such as exciton localization and self-trapping 16 , intrinsic Pb 2+ ion emissions 17 , and small-polaron generation 18 , are determined by the isolated [PbX6] 4octahedral units.…”
mentioning
confidence: 99%
“…The emergence of CsPbBr 3 MW waveguides has recently come to light and whilst they do share some similarities with our CsPbI 3 waveguides the mechanisms governing their behaviour at certain wavelengths appears markedly different. In the case of the CsPbBr 3 MWs reported elsewhere, 36 above bandgap (2.36 eV) excitation results in PL emission, where the authors indicate a photon recycling mechanism. This was built partly from spectral shifting observations as a function of distance along the MW, as well as former reports on the charging of perovskite surface layers.…”
Section: Communication Materials Advancesmentioning
confidence: 70%