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It must be noticed that p 3 ′ is always negative when p 5 is negative.
In (9), it can be noticed that P TxLR1 has been modified to P TxLR1_A and P TxLR1_B, while R LR1 has been modified to R LR1_A and R LR1_B to imply the possible different power requirements or different achieved data rates on the LR1 interface of different MTs, based on their position with respect to the LR1 AP.
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It is noticed that P V shows a decreasing trend with respect to the increasing values of λ, α, and v, but an increasing trend has been found with other parameters for both cases.
It can also be noticed that the p-value cutoffs were relatively stringent for the real data sets.
Although paper [6] complements [7], where the case p = 1 had been considered, it should be noticed that the case p = 1, A ≥ 1 is not dealt with in [6].
Finally, once the prediction filter p j ( H H ) is optimized and fixed, it can be noticed that the other prediction filters p j ( H L ) and p j ( L H ) can be separately optimized by minimizing J ℓ 1 ( p j ( H L ) ) and J ℓ 1 ( p j ( L H ) ) as explained in Section 3.
In order to find the eigenfunctions Ψ ( r e →, r h → ) of the exciton Hamiltonian (Equation 1), it must be noticed that the total in-plane exciton momentum P → ̂ = ( P ̂ x, P ̂ y ) is an exact integral of motion, and the exciton envelope wave function may be written as follows: Ψ ( r e →, r h → ) = exp ( i / ℏ ) ( P → · R → ) S ϕ ( ρ, z e, z h ), (3).
It should be noticed that the effects of initial stress P ∗ and magnetic field H 0 on the dimensionless frequency tend to be the increasing dimensionless frequency.
It has also to be noticed that, although increasing the block dimension P significantly improves mark imperceptibility, it does not affect negatively the mark extraction capability, making thus preferable the selection of large block values such as P=17.
It may be noticed that the decay of the induced discontinuity [p x ] is much slower than that of the decay of the shock.
It can be noticed that.
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