Ultrathin molybdenum oxide anode buffer layer for organic photovoltaic cells formed using atomic layer deposition
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Batteries based on Mg metal anode can promise much higher specific volumetric capacity and energy density compared to Li-ion systems and are, at the same time, safer and more cost-effective. While previous experimental reports have claimed reversible Mg intercalation into beyond Chevrel phase cathodes, they provide limited evidence of true Mg intercalation other than electrochemical data. Transmission electron microscopy techniques provide unique capabilities to directly image Mg intercalation and quantify the redox reaction within the cathode material. Here, we present a systematic study of Mg insertion into orthorhombic V 2 O 5 , combining aberration-corrected scanning transmission electron microscopy (STEM) imaging, electron energy-loss spectroscopy (EELS), and energy-dispersive X-ray spectroscopy (EDX) analysis. We compare the results from an electrochemically cycled V 2 O 5 cathode in a prospective full cell with Mg metal anode with a chemically synthesized MgV 2 O 5 sample. Results suggest that the electrochemically cycled orthorhombic V 2 O 5 cathode shows a local formation of the theoretically predicted ϵ-Mg 0.5 V 2 O 5 phase; however, the intercalation levels of Mg are lower than predicted. Lastly, this phase is different from the chemically synthesized sample, which is found to represent the δ-MgV 2 O 5 phase.
In this study, we presented structure-reactivity correlations for the gas-phase rate constants for hydrogen abstraction from sp3-hybridized carbon by three electrophilic radicals (X • + HCR 3 → XH + • CR 3 ; X = Cl • , HO • , and Br); the reaction enthalpy effect was represented by the independent variable Δ r H and the polar effect by the independent variables F and R, the Hammett-Taft constants for field/inductive and resonance effects. Here we present a parallel treatment for the less electronegative CH 3 • . In spite of a limited and scattered data base, the resulting least-squares fit [log k 437 (CH 3 • ) = 0.0251(Δ r H) + 0.96(ΣF) 0.56(ΣR) – 19.15] was modestly successful and useful for initial predictions. As expected, the polar effect appears to be minor and its directionality, i.e., the philicity of CH 3 , may depend on the nature of the substituents.