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Panel A illustrates that synchronization accuracy improves (mean signed asynchronies closer to zero when synchronizing to the beat) with increasing strength of selective neural entrainment to the beat.
The inset of (a) illustrates that the friction coefficient decreases from 1.3 ps-1 to a value in the order of 0.01 ps-1 when the temperature is increased from 25 to 200 K.
Figure 4(a) illustrates that even a polynomial of the fourth degree can conveniently be fitted to through, but difficulties (in terms of noisy behavior) obviously arise for the remaining parameter.
Effect of node speed on false positive rate is shown in Fig. 7 a, under the MATF and the SATF. Figure 7 a illustrates that false positive rate is much lower in the MATF as compared to the SATF.
Figure 5(a) illustrates that the hmF2 simulated by IRI and MAGIC are similar, expect IRI yielding a greater value near the magnetic equator at PIMO. Figure 5(b) further shows that both IRI and MAGIC fail to simulate the hmF2 eclipse and storm signatures.
Figure 4(a) illustrates that without time delay of matched filter but having the Doppler shift less than 1 unit, the autocorrelation value of optimized punctured ZCZPS falls sharply during one unit, and the trend of the amplitude over the whole frequency domain decreases as well.
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The dark field measurements in Figure 2 a d illustrate that, compared to solid spherical Au nanoparticles of similar size, the scattering of the Au nanosponges is red-shifted.
Here's a figure that illustrates that point.
Long ago, I had an experience that illustrates that point perfectly.
As the Compton case illustrates, that's a public health hazard and it ought to change.
Result presented in Figure 5(a) illustrated that, at zero time, high PPO activity was observed (29.10 U·g−1).
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com