Exact(5)
In trial 2, calves fed MR with Apex gained BW faster and were more efficient from 0 to 42 d than calves fed MR without Apex (P < 0.05).
Significant increases were reported for upper inter-incisal width apex (p < 0.001) and upper right first molar-lateroorbitale angle (p < 0.05) only in the RME group.
Significant increases were reported for upper inter-incisal width apex (p < 0.001) and upper right first molar-lateroorbitale angle (p < 0.05), only the RME group.
Calves fed MR with Apex gained BW faster from 0 to 35 d, were more efficient from 0 to 56 d, and consumed more starter from 42 to 56 d than calves fed MR without Apex (P < 0.05).
**p < 0.01 (comparing to the apex), ##p < 0.01 (comparing to LPN and H2O groups of the basal turn) (one-way ANOVA with LSD test used as post hoc analysis).
Similar(3)
Substitution of their result into the Eq. 12 leads to A_{{{text{dI}}/{text{dV}}}} = - P_{text{T}} P_{text{S}}, (13 which links the dI/dV asymmetry, A dI/dV, to the spin polarization of the sample at the tip apex position, P S(R T).
Assuming an adiabatic system (this process occurs in less than 40 ns; therefore, this assumption is reasonably accurate), the minimum required energy Em can be estimated using Equation 2: E m = m Au - NP C P, Au T m, Au - NP – T 0 + m apex C P, Si T m, Au - NP – T 0 = 4.27 × 10 - 15 J. (2).
The electric field amplitude of the incident light (│E i │), period (P), apex angle of antenna, antenna thickness (a), outline thickness (t), gap width (g), apex width (b), and area of gap region (A) are set to be │E i │ = 1 V/m, P = 775 nm, θ = 900, a = 35 nm, t = 10 nm, g = 30 nm, b = 30 nm and A = 30 × 30 nm2 throughout this paper unless otherwise specified.
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