2018
DOI: 10.1021/acsenergylett.8b01722
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Donor/Acceptor Charge-Transfer States at Two-Dimensional Metal Halide Perovskite and Organic Semiconductor Interfaces

Abstract: Metal halide perovskite semiconductors with small exciton binding energy have been widely used in perovskite solar cells and achieved rapid progress in terms of device performance. However, the strong excitonic nature of two-dimensional (2D) perovskites with small n values remains underexploited (n represents the number of inorganic monolayer sheets sandwiched between bulky organic cation layers). In this work, we report experimental evidence of donor/acceptor charge-transfer (CT) states formed at 2D metal hal… Show more

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Cited by 40 publications
(37 citation statements)
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“…27 The organic layer determines other properties of the hybrid 2DLP as well, such as its hydrophobicity and stability; 21,[28][29] structural rigidity; 20,30 sheetto-sheet distance; [31][32][33] and the dielectric screening experienced by charge carriers confined within the inorganic layer. [34][35][36] Early work focused primarily on n = 1 layered perovskites, in which the alternating stacks of organic cations surround atomically-thin inorganic sheets. 3,9,[37][38][39][40] However, recent work has extensively centered on variable well thickness in layered structures with n > 1, in particular the Ruddlesden-Popper-phase perovskites (RPPs, Figure 2a).…”
Section: Structural Diversity In Hybrid Materialsmentioning
confidence: 99%
“…27 The organic layer determines other properties of the hybrid 2DLP as well, such as its hydrophobicity and stability; 21,[28][29] structural rigidity; 20,30 sheetto-sheet distance; [31][32][33] and the dielectric screening experienced by charge carriers confined within the inorganic layer. [34][35][36] Early work focused primarily on n = 1 layered perovskites, in which the alternating stacks of organic cations surround atomically-thin inorganic sheets. 3,9,[37][38][39][40] However, recent work has extensively centered on variable well thickness in layered structures with n > 1, in particular the Ruddlesden-Popper-phase perovskites (RPPs, Figure 2a).…”
Section: Structural Diversity In Hybrid Materialsmentioning
confidence: 99%
“…(19,27) This finding would instead support type-I alignment between RDPs of increasing n. Furthermore, in alignment with this framework, Silver et al recently investigated the IE and EA of BTA n = 1 films by a mix of experimental and computational studies with the conclusion that n = 1 exhibits type-I alignment with MAPbX3 bulk perovskite. (22) These conflicting reports of type-I and type-II band alignments among RDPs have propagated in citing literature, leading to contradictory explanations for optoelectronic device performance across the perovskite research community, some attributing their performance to type-I alignments, (19,28,29) some attributing it to type-II alignments, (30−32) and some speculating that their devices are pure phase making RDP interfaces irrelevant. (3) One source of inconsistency in RDP band alignment studies could be attributed to film inhomogeneity.…”
Section: Single-crystal Band Levelsmentioning
confidence: 99%
“…This, in turn, results in a higher dielectric constant and reduces the exciton binding energy. [47,[75][76][77] This original approach opens a new way toward tailoring the optoelectronic properties of LPKs by using commercially available small dopants and the great variety of existing organic spacers. In the pioneering work by Passarelli et al a small organic electron-acceptor molecule, tetrachloro-1,2-benzoquinone TCBQ, was introduced to the organic layer formed by the naphthalene-based ammonium cations (Nap-O-R, R = ethylammonium, propylammonium, butylammonium, hexylammonium).…”
Section: Lead Halide Bond Distortionmentioning
confidence: 99%