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According to the results in Fig. 4, a calibration was carried out to exclude the contributions of surface potential difference and Van der Waals' force.
According to the experimental results in Fig. 4, a calibration was conducted to exclude the contributions of surface potential difference and Van der Waals' force.
The perovskite BFO enhances the fluorescence intensity (at 660 and 832 nm) and surface potential difference (−469 ~ 385 meV and −80 ~ 525 meV) of the embedded spinel XFO.
The formation of Ti-Al intermetallic interlayer and Al diffusion layer at interface effectively reduced the surface potential difference at the interface.
The results revealed that the perovskite BiFeO3 enhances the fluorescent intensity (at 635 and 795 nm) and surface potential difference (14 meV and −40 meV) of the embedded spinel (XZn)Fe2O4.
The origin of the high/low photovoltage response region (theoretical difference data ~200 meV; experimental difference data 45~160 meV) is attributed to the surface potential difference (270 meV/3~70 meV) of Fe2O3 and XFe2O4, according to the theoretical potential images (see Fig. 3c).
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In summary, we showed that thiol SAM pattern with chemical functionality and desired surface potential differences can be created using AFM-based nanografting method.
EIT data were generated by application of electrical alternating current (50 kHz, 5 mA peak-to-peak) in a sequential rotating process and measurement of the resulting surface potential differences between neighboring electrode pairs was performed.
In this work, we proposed a planar nano-gap structure for surface-potential difference monitoring.
Based on the proposed architecture, the variance of surface-potential difference can be determined by electrical double layer capacitance (EDLC) between the nano-gap electrodes.
First, the surface contact potential difference (CPD) strongly increases inside the GO flake and reaches the maximum value about 160 mV at 140 °C annealing.
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