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By increasing the amount of graphene in the suspension, the intensity of SPR peak in the absorption spectrum decreased and the width of the peak increased.
Thus, FA intensity was relatively enhanced compared to D0X and TES as increasing temperature, though the absolute intensity of whole spectrum decreased.
However, all the bands in the Ag-Pal nanocomposite spectrum decreased in intensity, compared to those of the Pal matrix, indicating that the Ag NPs interacted with the surface of the Pal support.
In this long-time period (Fig. 8, between t 1 and t 2 moments), the ML changed its position in the region of 550 450 eV and had not vanished; however, its moving rate along the spectrum decreased down to RM = 0.4 eV/min.
Later, the far-UV CD spectrum decreased in intensity, suggesting the appearance of larger aggregates (Fig. 7A).
In normal conditions, the firing rate power spectrum decreased as 1/f (Figure 8E and 8F, black traces) for frequencies between 0.1 and 1 Hz as shown above.
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In these models, the power-law index of the primordial power spectrum decreases with increasing wavenumber.
It is found that the resonant frequencies increase as the material stiffness increases or the tip mass decreases, and the spectrum decreases by increasing the damping.
In order to eliminate the shift of the transmission spectrum, decrease the crosstalk, and further realize the accurate demultiplexing, the redesign of the AWG device is carried out.
The relative strength of the alumina signature to the spectrum decreases with increasing mass-loss rate, suggestive of a covering of the alumina grains by silicate mantles.
Because the neutrino spectrum decreases strongly with increasing energy, most of the rate will be near the lower end of this range.
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