3 research outputs found

    Source of Electrofreezing of Supercooled Water by Polar Crystals

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    Polar crystals, which display pyroelectricity, have a propensity to elevate, in a heterogeneous nucleation, without epitaxy, the freezing temperature of supercooled water (SCW). Upon cooling, such crystals accumulate an electric charge at their surfaces, which creates weak electric fields, –1, that are thousands of times lower than necessary for inducing homogeneous ice nucleation. By performing comparative freezing experiments of SCW on the same surfaces of three different polar crystals of amino acids, we demonstrate that preventing the formation of charge at these surfaces, by linking the two hemihedral faces of the polar crystals with a conducting paint, reduces the temperature of freezing by 2–5 °C. The temperature of ice nucleation was found to be correlated with the amount of the surface charge, thus implying that the surface-charge-induced interactions affect the interfacial water molecules that trigger freezing at a higher temperature. This finding is in contrast to previous hypotheses, which attribute the enhanced SCW freezing to the effect of the electric field or capture of external ions or particles. Possible implications of this mechanism of freezing are presented

    Impedance Spectroscopic Indication for Solid State Electrochemical Reaction in (CH<sub>3</sub>NH<sub>3</sub>)PbI<sub>3</sub> Films

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    Halide perovskite-based solar cells still have limited reproducibility, stability, and incomplete understanding of how they work. We track electronic processes in [CH<sub>3</sub>NH<sub>3</sub>]­PbI<sub>3</sub>(Cl) (“perovskite”) films <i>in vacuo</i>, and in N<sub>2</sub>, air, and O<sub>2</sub>, using impedance spectroscopy (IS), contact potential difference, and surface photovoltage measurements, providing direct evidence for perovskite sensitivity to the ambient environment. Two major characteristics of the perovskite IS response change with ambient environment, viz. -1- appearance of negative capacitance <i>in vacuo</i> or post<i>-vacuo</i> N<sub>2</sub> exposure, indicating for the first time an electrochemical process in the perovskite, and -2- orders of magnitude decrease in the film resistance upon transferring the film from O<sub>2</sub>-rich ambient atmosphere to vacuum. The same change in ambient conditions also results in a 0.5 V decrease in the material work function. We suggest that facile adsorption of oxygen onto the film dedopes it from n-type toward intrinsic. These effects influence any material characterization, i.e., results may be ambient-dependent due to changes in the material’s electrical properties and electrochemical reactivity, which can also affect material stability

    Local Environment of Sc and Y Dopant Ions in Aluminum Nitride Thin Films

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    The local environments of Sc and Y in predominantly ⟨002⟩ textured, Al1–xDoxN (Do = Sc, x = 0.25, 0.30 or Y, x = 0.25) sputtered thin films with wurtzite symmetry were investigated using X-ray absorption (XAS) and photoelectron (XPS) spectroscopies. We present evidence from the X-ray absorption fine structure (XAFS) spectra that, when x = 0.25, both Sc3+ and Y3+ ions are able to substitute for Al3+, thereby acquiring four tetrahedrally coordinated nitrogen ligands, i.e., coordination number (CN) of 4. On this basis, the crystal radius of the dopant species in the wurtzite lattice, not available heretofore, could be calculated. By modeling the scandium local environment, extended XAFS (EXAFS) analysis suggests that when x increases from 0.25 to 0.30, CN for a fraction of the Sc ions increases from 4 to 6, signaling octahedral coordination. This change occurs at a dopant concentration significantly lower than the reported maximum concentration of Sc (42 mol % Sc) in wurtzite (Al, Sc)N. XPS spectra provide support for our observation that the local environment of Sc in (Al, Sc)N may include more than one type of coordination
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