1,721,266 research outputs found

    Publishing Hybrid/Organic Photovoltaics Papers in ACS Energy Letters

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    With the swift surge of organohalide metal perovskites as a major player in the arena of emerging photovoltaic technologies, the field of traditional Hybrid/Organic Photovoltaics (HOPV) has been profoundly modified. By traditional HOPV, here we mean dye-sensitized solar cells (DSCs), bulk heterojunction or small-molecule organic solar cells (OSCs), and quantum dot solar cells (QSCs). These technologies dominated publications in basic and applied science journals up to 2012, when the perovskite storm started with the first reports of high-efficiency solid-state perovskite solar cells.1,2 Despite being initially based on a typical DSC architecture,3 perovskite solar cells have outperformed their DSC ancestor in about 2 years from their inception, demonstrating a high efficiency (>22%) in a variety of solid-state device architectures, ranging all the way from a planar to a mesoscopic heterojunction. Since 2012, traditional HOPV technologies have been somehow lying in the shadow of the perovskite giant, mainly due to the efficiency gap between traditional HOPV (topping after 2 decades of research at 11− 14%) and perovskite solar cells

    Perovskite Solar Cells on Their Way to the Market

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    I recently attended the third Perovskite Solar Cells and Optoelectronics (PSCO) conference, which was held September 18−20, 2017 in Oxford (U.K.). Along with Henry Snaith, Md. K. Nazeeruddin, and Annamaria Petrozza, I served as one of the co-Organizers of this meeting. The conference was an occasion to interact with nearly 400 attendees and capture the latest advances from international researchers (∼100 oral and ∼170 poster presentations) in the metal-halide perovskites field, including the Perovskite Death Starlet, see Figure 1. This PSCO conference became a cornerstone, at least in my perception, of how far and how quickly the perovskite field has advanced toward the launch of a possible industrial product. Although most of the presentations were devoted to basic science, including elaborate theoretical chemistry, materials science, and solid-state physics concepts, discussions and presentations related to practical applications were prominent. This evolution of the theme, I believe, is a kind of unique aspect of perovskites, which have raised tremendous interest both from fundamental academic and industrial perspectives. While basic science studies continue to reveal the factors behind the intriguing properties of perovskite materials, several companies worldwide are progressing toward the launch of perovskite solar cell panels in the market. Today, the debate centers on whether perovskites will make their way through the photovoltaic market as standalone devices, or whether tandem devices with silicon (or other established technologies) will be the first perovskite products to be launched. To give an account of the latest industrial developments in perovskite solar cells, I have gathered a few quotes from the representatives of three industrial participants at PSCO: “The recent, very successful PSCO 2017 conference supports the view of Oxford PV that perovskite-based PV has made substantial progress towards industrialization. As The Perovskite Company, we are working to demonstrate a full silicon− perovskite solar cell at our facility in Brandeburg an der Havel, a key step on the path to commercialize this important technology.” Chris Case, Chief Technology Officer, Oxford Photovoltaic

    Alignment of the dye's molecular levels with the TiO(2) band edges in dye-sensitized solar cells: a DFT-TDDFT study

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    We present a theoretical study of the lineup of the LUMO of Ru(II)-polypyridyl (N3 and N719) molecular dyes with the conduction band edge of a TiO(2) anatase nanoparticle. We use density functional theory (DFT) and the Car-Parrinello scheme for efficient optimization of the dye-nanoparticle systems, followed by hybrid B3LYP functional calculations of the electronic structure and time-dependent DFT (TDDFT) determination of the lowest vertical excitation energies. The electronic structure and TDDFT calculations are performed in water solution, using a continuum model. Various approximate procedures to compute the excited state oxidation potential of dye sensitizers are discussed. Our calculations show that the level alignment for the interacting nanoparticle-sensitizer system is very similar, within about 0.1 eV, to that for the separated TiO(2) and dye. The excellent agreement of our results with available experimental data indicates that the approach of this work could be used as an efficient predictive tool to help the optimization of dye-sensitized solar cells

    Unraveling Atomic Contributions to the London Dispersion Energy: Insights into Molecular Recognition and Reactivity

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    We present a general framework that enables quantification with atomic resolution of the overall London dispersion energy, which can be readily integrated with currently available energy decomposition schemes. This approach can be used to determine the contribution of individual atoms and functional groups to molecular recognition, conformational preferences, molecular stability, and reactivity. Its efficacy across diverse realms of molecular chemistry and biology is demonstrated with application to molecular balances in solution, asymmetric organocatalytic transformations, and a subcomplex of the F1FO ATP synthase

    Full Quantum Mechanical Investigation of the Unimolecular versus Bimolecular Acetylene to Vinylidene Rearrangement in the Prototypetrans-Cl-Rh(Pi-Pr3)2Complex

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    We report a full quantum mechanical investigation, based on DFT calculations, on the unimolecular and bimolecular alkyne-vinylidene rearrangements in the prototype [Cl-Rh(Pi-Pr-3)(2)(HC CH)] complex, to solve the discrepancy between theory and recent experimental data and to provide a definitive answer concerning the largely debated molecularity issue of the 1,3-shift in d(8) metal complexes. We calculate the intramolecular pathway to be kinetically favored over the intermolecular one by 15.0 kcal/mol, in agreement with recent crossover experiments. Comparison of our DFT calculations performed on the real systems with reduced models shows that a full quantum mechanical description of the investigated systems is mandatory for a correct description of their reactivity, owing to the relevant role played by the electron-donating phosphine ligands

    Time-dependent density functional theory study of the absorption spectrum of [Ru(4,4′-COOH-2,2′-bpy)2(NCS)2] in water solution: Influence of the pH

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    We present a combined density functional/time-dependent density functional study of the electronic structure and optical absorption spectrum of the charge-transfer sensitizer cis-[Ru(4,4'-COOH-2,2'-bpY)(2)(NCS)(2)] in water solution. To simulate the effect of different pH values, calculations have been performed for both the title complex and the corresponding tetra-deprotonated species, cis-[Ru(4,4'-COO-2,2'-bPY)(2)(NCS)(2)](4-). The experimentally observed blue-shift of the spectrum at high pH is well reproduced by our theoretical model and appears to be related to destabilization of the bipyridines pi(*) LUMOs as a result of the increased electron density on the deprotonated carboxylic groups. (C) 2004 Elsevier B.V. All rights reserved

    Correction to “Computational Investigation of Dye–Iodine Interactions in Organic Dye-Sensitized Solar Cells”

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    We present a computational investigation, based on DFT, MP2, and Car−Parrinello molecular dynamics simulations, aimed to model the dye−iodine interactions in organic dyesensitized solar cells. We evaluate the binding of I2 and I3 − and Li+ to the various electron-donating sites in organic sensitizers considering two coumarin dyes differing by the number of thiophene rings in the bridge (NKX2587 vs NKX2697) and one carbazole dye (MK3), which have been the subject of a detailed experimental investigation (J. Am. Chem Soc. 2008, 130, 17874− 17881). We find that oxygen atoms are the preferred binding sites for I2, while I3 − tends to interact with the π system of the coumarin donor unit. Our results suggest that the increase of the distance of the carbonyl oxygen from the titania going from NKX2587 to NKX2697 could explain the differences in the lifetime values measured for NKX2587-sensitized solar cells compared to those employing the longer NKX2697 homologues. The shorter lifetime measured for MK3 compared to NKX2687, which have the same π-spacer and acceptor units, is instead attributed to the twisting of the dye structure in MK3, which possibly forms less compact dye layers on titania. The effect of the dye structure and Li+ coordination to the dyes on the titania conduction band is also examined

    Structural and electronic properties of organo-halide hybrid perovskites from ab initio molecular dynamics

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    The last two years have seen the unprecedentedly rapid emergence of a new class of solar cells, based on hybrid organic–inorganic halide perovskites. The success of this class of materials is due to their outstanding photoelectrochemical properties coupled to their low cost, mainly solution-based, fabrication techniques. Solution processed materials are however often characterized by an inherent flexible structure, which is hardly mapped into a single local minimum energy structure. In this perspective, we report on the interplay between structural and electronic properties of hybrid lead iodide perovskites investigated using ab initio molecular dynamics (AIMD) simulations, which allow the dynamical simulation of disordered systems at finite temperature. We compare the prototypical MAPbI3 (MA = methylammonium) perovskite in its cubic and tetragonal structure with the trigonal phase of FAPbI3 (FA = formamidinium), investigating different starting arrangements of the organic cations. Despite the relatively short time scale amenable to AIMD, typically a few tens of ps, this analysis demonstrates the sizable structural flexibility of this class of materials, showing that the instantaneous structure could significantly differ from the time and thermal averaged structure. We also highlight the importance of the organic–inorganic interactions in determining the fluxional properties of this class of materials. A peculiar spatial localization of the valence and conduction band edges is also found, with a dynamics in the range of 0.1 ps, which is associated with the positional dynamics of the organic cations within the cubo-octahedral perovskite cage. This asymmetry in the spatial localization of the band edges is expected to ease exciton dissociation and assist the initial stages of charge separation, possibly constituting one of the key factors for the impressive photovoltaic performances of hybrid lead-iodide perovskites
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