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Besides, the electrode displayed two flat potential profiles during the charge/discharge process.
Namely, it is resultant from the flat potential energy surface due to the occupation of electrons on both the bonding and anti-bonding states, which leads to a strong competition and frustration between electron localization and delocalization.
Its relatively flat potential means that it will typically acquire a large vacuum expectation value during inflation, ushering in a post-inflationary epoch of relaxation.
It was known that the conduction band potentials of n-type semiconductors were closed to the flat potential [39, 79, 80].
Additionally, a remarkable cathodic shift in the flat potential from 0.44 V for TiO2 sample to 0.36 V for the CdS/Fe2O3/TiO2 NR sample was observed.
Typical charge and discharge curves of the RE-perovskite-type electrodes show long and flat potential plateaus, Fig. 4a, b, which represents the interaction between hydrogen atoms and oxygen in the oxide during the absorption/desorption process [27, 78].
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Importantly, in pyramidal II slip plane, a flat potential-energy surface (PES) exists around the position of stable stacking fault energy (SFE), which allows cooperative movement of atoms within the slip plane.
Mott-Schottky plots based on Nyquist plots at various potentials gave the flat band potential of 0.62 V (vs. Ag/AgCl) at pH 6.0.
Furthermore, the flat band potential of the oxide, which separates potential regions of predominant ionic conduction from regions of predominant electronic conduction, can be considered a critical potential.
In the dark, the flat band potential (measured by Mott Schottky technique) and the onset potential were shifted by up to 300 mV depending on surface charge density.
The flat band potential increases with an increase in the film formation potential.
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