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It is possible to obtain orthogonal space-time codes for three transmit antennas, which in our case correspond to the antennas at the three neighboring BSs.
Since the Hall effect measurements in this case correspond to the region of mixed conductivity, it is not possible to determine the charge carrier concentrations.
The routing tree for Node 0 at t=0 is identical to the one depicted in Fig. 2 because exact schedules in the scheduled one-time connection case correspond to initial wait times in the periodic connection case.
The features in this case correspond to the spatial grid on which measurements are performed (i.e., (x,y) or (x,y,z)), whereas samples correspond to wavelength, energy, voltage, mass-to-charge ratio, etc.
The various traces in each case correspond to different λ p over a time span of 10 to 500 ps and were obtained using a fluence of 115 μJ/cm2.
That is, for the three possible ordered alternatives (for k = 1, 2, 3), which in our case correspond to the employment statuses mentioned above, we observe l it = k if μk−1 < l it * ≤ μ k, where μ0 = −∞ and μ m = ∞, with m being the number of alternatives.
Similar(48)
This case corresponds to Figure11a.
Here α=0 case corresponds to RW sampling.
This case corresponds to implying (59).
Case 2. This case corresponds to, meaning (65).
This case corresponds to absence of any resonances.
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