2022
DOI: 10.1103/physrevlett.129.177401
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Ultrafast Excitonic Response in Two-Dimensional Hybrid Perovskites Driven by Intense Midinfrared Pulses

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Cited by 9 publications
(9 citation statements)
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“…These solution-processed films, despite the presence of cracks that are spaced hundreds of microns apart, still exhibit good uniformity within each domain and feature large grain sizes. The reflectance spectra of both samples shown in Figure b exhibit pronounced reflection dips around 500 nm, which are characteristic of exciton resonances in these materials. The exciton resonance in (PEA) 2 PbI 4 is slightly red-shifted compared to (BA) 2 PbI 4 . The reflection dips at wavelengths beyond 520 nm, which fall below the absorption spectral window, are attributed to interference fringes …”
Section: Resultsmentioning
confidence: 98%
See 1 more Smart Citation
“…These solution-processed films, despite the presence of cracks that are spaced hundreds of microns apart, still exhibit good uniformity within each domain and feature large grain sizes. The reflectance spectra of both samples shown in Figure b exhibit pronounced reflection dips around 500 nm, which are characteristic of exciton resonances in these materials. The exciton resonance in (PEA) 2 PbI 4 is slightly red-shifted compared to (BA) 2 PbI 4 . The reflection dips at wavelengths beyond 520 nm, which fall below the absorption spectral window, are attributed to interference fringes …”
Section: Resultsmentioning
confidence: 98%
“…We attribute this observed transient response to the heat-induced broadening of the exciton resonance, a phenomenon we recently demonstrated for (BA) 2 PbBr 4 under MIR vibrational excitation. 36 In essence, lattice heating enhances electron−phonon interactions, leading to a stronger damping factor for the exciton resonance. 46 The rapid, subnanosecond interband carrier relaxation times and the nanosecond time resolution of our PPM setup prevent us from observing the initial blue shift under 380 nm excitation and the electronic dynamics in these strongly excitonic materials.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…Instances involving OIHPs with n = 1 often exhibit robust quantum and dielectric confinement effects, accompanied by a somewhat subdued photoluminescence, often attributed to Auger recombination . A more in-depth understanding of Auger recombination hinges on a thorough delineation of quantum and dielectric confinement facilitated by 2D structures. , There is a growing anticipation for the development of advanced characterization techniques tailored for OIHPs, which not only enrich the understanding of dielectric-related phenomena but also serve as a theoretical compass for practical applications of these OIHPs.…”
Section: Discussionmentioning
confidence: 99%
“…[31] In contrast, 2D layered perovskite materials have a multiple quantum well-like structure with general formula (A´) m A n-1 B n X 3n+1 , where A´is bulky cations that form a monolayer or bilayer connecting the conductor (A) n-1 B n X 3n+1 2D sheets. [32][33][34] 2D perovskite structures are mostly categorized into Ruddlesden-Popper (R-P) and Dion-Jacobson (D-J) phases. [35] The optoelectronic properties of 2D halide perovskites can be synergistically tuned by the number of inorganic layers and by changing the size, shape, charge, and location of bulky organic cations.…”
Section: Introductionmentioning
confidence: 99%