2018
DOI: 10.1002/adom.201700975
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Excitations Partition into Two Distinct Populations in Bulk Perovskites

Abstract: Organolead halide perovskites convert optical excitations to charge carriers with remarkable efficiency in optoelectronic devices. Previous research predominantly documents dynamics in perovskite thin films; however, extensive disorder in this platform may obscure the observed carrier dynamics. Here, carrier dynamics in perovskite single‐domain single crystals is examined by performing transient absorption spectroscopy in a transmissive geometry. Two distinct sets of carrier populations that coexist at the sam… Show more

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Cited by 9 publications
(17 citation statements)
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“…Material constants derived from the fits are tabulated in Table I Based on V p , the polaron radius in bulk CsPbBr 3 and the CsPbBr 3 NCs is 12.1 and is 11.9 nm, respectively. Although "large" polarons are often invoked to explain the unique photophysics of LHPs, [31][32][33][34][35][36][37][38] we note these values are approximately double to the polaron size experimentally determined by Munson et al for MAPbI 3 (∼4.5 nm radius), 39 and larger still for the computationally-derived values for CsPbBr 3 reported elsewhere. 16,33 We posit that the relatively large values obtained here are a consequence of energy transfer processes which lead to an incorrect estimation of the local carrier density.…”
Section: Kinetic Modellingsupporting
confidence: 51%
“…Material constants derived from the fits are tabulated in Table I Based on V p , the polaron radius in bulk CsPbBr 3 and the CsPbBr 3 NCs is 12.1 and is 11.9 nm, respectively. Although "large" polarons are often invoked to explain the unique photophysics of LHPs, [31][32][33][34][35][36][37][38] we note these values are approximately double to the polaron size experimentally determined by Munson et al for MAPbI 3 (∼4.5 nm radius), 39 and larger still for the computationally-derived values for CsPbBr 3 reported elsewhere. 16,33 We posit that the relatively large values obtained here are a consequence of energy transfer processes which lead to an incorrect estimation of the local carrier density.…”
Section: Kinetic Modellingsupporting
confidence: 51%
“…Similarly, the effects of electronic confinement and carrier trapping on carrier relaxation in LHPs are still under debate, not least because of the elaborate photophysics which occur in these materials and inhibit the contributions of specific effects toward carrier cooling from being studied in a controlled and isolated fashion. 26,[57][58][59] In this work, we evaluate the impact of the hot and cold carriers, as well as surface and confinement effects, on the hot carrier relaxation dynamics in LHP NC solids. For this we apply a three-pulse "pump-push-probe" (PPP) experiment, where the density of the hot and cold carrier subensembles are individually controlled.…”
mentioning
confidence: 99%
“…5 Long charge carrier lifetimes, ranging from a few to hundreds of nanoseconds, have been reported for hybrid perovskites. 9,10 Explanations for such long carrier lifetimes include unusual defect tolerance, 11−14 formation of polarons, 15,16 direct-to-indirect bandgap transition, 17,18 fast carrier relaxation enabled by spin−orbit interactions, 19 Rashba splitting, 20,21 and ferroelectric domains. 22 Most of these perovskite features are believed to correlate with the unique organic−inorganic hybrid perovskite structure.…”
mentioning
confidence: 99%