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The Friedman method shows the shift of a chemical control reaction to a diffusion control reaction due to the change of viscosity during the curing process.
Inset shows the shift of ruby fluorescence line with applied magnetic field.
Open image in new window Fig. 4 a Temperature-dependent PL spectra of the In0.65Ga0.35As nanowires under the same laser excitation, the dashed line shows the shift of the PL peak energy with changing the temperature.
Figure 3 shows the shift of TB towards a lower temperature (TB = 170 to 55 K) with increasing distance between the iron oxide particles with a diameter of 8 nm by changing the concentration of the Fe3O4 solution from 8too 2 mg Fe/ml.
To reveal the mechanism of the doping effect on HER performance, the partial density of states is calculated and shows the shift of the Fermi level as the hydrogen coverage increases (Figs. 5 and 6; Additional file 1: Figures S4 S7).
Figure 4 shows the shift of TB to a lower temperature, from 160 to 130 K, with decreasing pore diameter (from 90 to 50 nm) and increasing distance between the pores (from 35 to 50 nm) in the porous silicon matrix.
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(b) The magnification of Fig. 2a, showing the shift of the redox peaks of Ni over the course of 18 h.
FTIR spectra of PC compared to the carbon films show the shift of maximum absorbency from sp3 CH3 to sp3 CH2 in the range of 2970 2920 cm−1.
Five figures show the shift of feature distribution by changing the volume of the drum part.
The latter showed the shift of XRD peak positions to higher diffraction angles in comparison with those of Cu-free Y-doped ZrO2 samples.
Kelvin probe force microscopy results evidently show the shift of Fermi level in different ZnO films and are well associated with the changing of carrier concentration.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com