Figure 8 shows the decision variable as a function of the input SNR (under AWGN conditions) for several values of.
So, we experimented with several values of the smoothing factors and empirically optimized them under the MI measure.
In Fig. 14, the capacity under TCIFR policy, given in (49), is traced versus L for β=2.8,φ=−0.223, and several values of a fixed cutoff fade depth γ ∗.
Then, we experimented with several values of N ESN to form different EESNs and evaluated them under the estimation error of the HF spectral envelope.
Several values of (kappa ) are shown.
Several values of site_p were tried.
The second group of experiments is used to compare the performance metrics of cellular downlink throughput, average delay, and network connectivity ratio of DTO-MROD under several typical values of discount coefficient η and RIE threshold.
In Figure 2, we plot the spin-dependent transmission probability τ σ, spin-dependent See-beck coefficient S σ, and spin-dependent Lorenz number L σ = h ( κ e l, σ T + κ e l, σ V ) ∕ ( e 2 τ σ T ) as functions of the chemical potential μ under several different values of ϕ at room temperature (T = 300 K).
The results indicate that a near pure spin thermoelectric generator can be obtained by tuning the AB phase ϕ with a fixed value of ϕ R. Figure 3 (Color online) Spin-dependent electronic thermal conductance κ e l, σ V and κ e l, σ T, charge FOM ZC T and spin FOM Z S T as function of the chemical potential μ under several different values of ϕ at room temperature (T = 300 K).
The corresponding q +↓ and |q -↑ | decrease, while q +↑ and |q -↓ | increase as λ increases (see table 2). Figure 5 (Color online) Spin-dependent electronic thermal conductance κ e l, σ V and κ e l, σ T, charge and spin figure of merit Z C T and Z S T as function of the chemical potential μ under several different values of λ at room temperature (T = 300 K).
