
Xingxing Zhang
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Effects of Cd Diffusion and Doping in High-Performance Perovskite Solar Cells Using CdS as Electron Transport Layer
IR and UV-NIR Absorption Spectroscopy of Matrix-Isolated C70+ and C70–
Robust Cross-Linked Stereocomplexes and C60 Inclusion Complexes of Vinyl-Functionalized Stereoregular Polymers Derived from Chemo/Stereoselective Coordination Polymerization
High Energetic Polymeric Nitrogen Stabilized in the Confinement of Boron Nitride Nanotube at Ambient Conditions
Controlled Sulfidation Approach for Copper Sulfide–Carbon Hybrid as an Effective Counter Electrode in Quantum-Dot-Sensitized Solar Cells
Passivation of Nickel Vacancy Defects in Nickel Oxide Solar Cells by Targeted Atomic Deposition of Boron
Interface-Dependent Ion Migration/Accumulation Controls Hysteresis in MAPbI3 Solar Cells
Efficient Photoinduced Charge Separation in a BODIPY–C60 Dyad
Stabilization of a Chlorinated #4348C66:C2v Cage by Encapsulating Monometal Species: Coordination between Metal and Double Hexagon-Condensed Pentalenes
Structural Changes in the Local Environment of Uranium Atoms in the Three Phases of U4O9
The dipolar endofullerene HF@C60

Nature Chemistry. doi:10.1038/nchem.2563
Authors: Andrea Krachmalnicoff, Richard Bounds, Salvatore Mamone, Shamim Alom, Maria Concistrè, Benno Meier, Karel Kouřil, Mark E. Light, Mark R. Johnson, Stéphane Rols, Anthony J. Horsewill, Anna Shugai, Urmas Nagel, Toomas Rõõm, Marina Carravetta, Malcolm H. Levitt & Richard J. Whitby
Hydrogen fluoride has been encapsulated in C60-fullerene using molecular surgery. The quantum rotor system has been studied by NMR and infrared spectroscopy as well as neutron scattering. The fullerene cage causes a small red-shift in the HF rotational and vibrational constants, and shields around 75% of its dipole.
Photoinduced Charge Separation in the Carbon Nano-Onion C60@C240
The Nature of the Noncovalent Interactions between Benzene and C60 Fullerene
Marcus Bell-Shaped Electron Transfer Kinetics Observed in an Arrhenius Plot
Charge Transfer Complexation of Ta-Encapsulating Ta@Si16 Superatom with C60
Correlating Surface-Functionalization of Mesoporous Silica with Adsorption and Release of Pharmaceutical Guest Species
High-efficiency two-dimensional Ruddlesden–Popper perovskite solar cells
Nature advance online publication 06 July 2016. doi:10.1038/nature18306
Authors: Hsinhan Tsai, Wanyi Nie, Jean-Christophe Blancon, Constantinos C. Stoumpos, Reza Asadpour, Boris Harutyunyan, Amanda J. Neukirch, Rafael Verduzco, Jared J. Crochet, Sergei Tretiak, Laurent Pedesseau, Jacky Even, Muhammad A. Alam, Gautam Gupta, Jun Lou, Pulickel M. Ajayan, Michael J. Bedzyk, Mercouri G. Kanatzidis & Aditya D. Mohite
Three-dimensional organic–inorganic perovskites have emerged as one of the most promising thin-film solar cell materials owing to their remarkable photophysical properties, which have led to power conversion efficiencies exceeding 20 per cent, with the prospect of further improvements towards the Shockley–Queisser limit for a single‐junction solar cell (33.5 per cent). Besides efficiency, another critical factor for photovoltaics and other optoelectronic applications is environmental stability and photostability under operating conditions. In contrast to their three-dimensional counterparts, Ruddlesden–Popper phases—layered two-dimensional perovskite films—have shown promising stability, but poor efficiency at only 4.73 per cent. This relatively poor efficiency is attributed to the inhibition of out-of-plane charge transport by the organic cations, which act like insulating spacing layers between the conducting inorganic slabs. Here we overcome this issue in layered perovskites by producing thin films of near-single-crystalline quality, in which the crystallographic planes of the inorganic perovskite component have a strongly preferential out-of-plane alignment with respect to the contacts in planar solar cells to facilitate efficient charge transport. We report a photovoltaic efficiency of 12.52 per cent with no hysteresis, and the devices exhibit greatly improved stability in comparison to their three-dimensional counterparts when subjected to light, humidity and heat stress tests. Unencapsulated two-dimensional perovskite devices retain over 60 per cent of their efficiency for over 2,250 hours under constant, standard (AM1.5G) illumination, and exhibit greater tolerance to 65 per cent relative humidity than do three-dimensional equivalents. When the devices are encapsulated, the layered devices do not show any degradation under constant AM1.5G illumination or humidity. We anticipate that these results will lead to the growth of single-crystalline, solution-processed, layered, hybrid, perovskite thin films, which are essential for high-performance opto-electronic devices with technologically relevant long-term stability.


























