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Since a scattering probability is inversely proportional to the mean-free time [24], the total scattering probability of a single hole carrier in nanowire channels (P SCAT) becomes as shown in Eq. 1: P_{text{SCAT}} simeq frac{1}{tau} = frac{1}{tau_{text{PH}}} + frac{1}{tau_{text{SRS}}}, (1).
Since for the conditions of this study the inventoried volume is the total bole, BEF becomes as shown by the following ratio: B E F = W c r o w n + W b o l e W b o l e = W a b o v e g r o u n d W b o l e. where: BEF = biomass expansion factor (dimensionless); W crown = tree crown dry weight (g), composed of foliage, thick and thin branches; W bole = tree bole dry weight (g); and.
Similar(58)
The competition of them makes the critical supercurrent becomes small, but the oscillatory amplitude becomes large as shown in Figure 3a.
Consequently, the mode volume of nanocavity mode becomes large, as shown in Figure 2c.
Because of this, pressure becomes weak, as shown in Figure 6(c).
As the substrate temperature increases, the density of InN nanodots becomes lower as shown in Fig. 7c.
For that reason, the delivery cost declines and the delay becomes longer, as shown in Fig. 7b, c, respectively.
When the foothold of leg (L_1) collapses, the ground reaction becomes zero, as shown with the black circle.
However, when the number of transmitters reaches a certain threshold, the situation becomes opposite, as shown in the figure.
However, as the unevenness in node distribution increases, the reduction in the PIT becomes less, as shown in Fig. 9a, b.
Indeed, a detailed investigation of the locality properties of the theory becomes possible as shown by Bell himself (Bell 1987, p. 47).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com