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The IIaex_IIa-1 had significant negative values for Fu's FS for both markers, although Tajima's D was not significant.
There were no differences for any of the measurements or time indices between the sheep (p = 0.37-0.85) and goats (p = 0.21-0.67) except for FS for both sheep and goats (p < 0.03).
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The behavior of ( u_{0} ) with respect to ( f ) for both slow and fast modes is depicted in Fig. 5.
Unlike in the situation with fixed n and γ→∞, for n→∞ we find fairly good tail behavior of LSE for normal F, for both fixed and random designs, even under heavy-tailed distribution for Xn.
The second one is the Absolute Scalar Magnetometer (ASM) and aims at providing very accurate 1 Hz absolute scalar measurements F for both scientific and VFM calibration purposes.
As we want to compare the performances, it is natural to take the same smoothing parameters K e, K r and K f for both of the methods.
At the final stage of the growth after 15 min, the coverage density has increased (Fig. 6e, f) for both types of solutions.
At 664 nm, the absorption for samples "f" for both NC sizes was less than those of samples "g", despite the fact that the concentration of the dye in these samples was the same.
Figure 4 shows the relationship between applied stress and t ss/t f for both Ni3(Si,Ti) and Ni3(Si,Ti) with 2Mo in 0.5 kmol/m3 NaCl solution at 313 K.
In addition, Fig. 6c shows the response of system against varying the values of R f for both the TMFD systems, keeping the optimum value of tuning frequency ratio and frequency spacing constant.
From Fig. 13, t ss/t f for both compounds was almost constant independent of pH in region B and was the same high value of 0.98 ± 0.02 as those in Figs. 4, 7, and 10.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com