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Let ({varepsilon }_{infty downarrow }^{text {out}}) be the minimum value of the energy ({varepsilon }_{infty }^{text {out}}(x)), that is: varepsilon_{inftydownarrow}^{text{out}} =min {{varepsilon}_{infty}^{text{out}}(x):xin {mathcal {X}}(mathcal{S}_{{o}},mathcal{S}_{{b}})} (17).
(P_{text {out}}^{l}) Outage probability constraint for layer l.
Using the fact that (left (1-mathcal {P}_{text {out}}^{text {off}}right) rightarrow 1) for high SNR, the asymptotic outage probability of T1 can be expressed as mathcal{P}_{text{out}}^{T_{1}} simeq left(mathcal{P}_{text{out}}^{text{off}}right)^{K} mathcal{P}_{text{out}}^{T_{1}T_{2}} + mathcal{P}_{text{out}}^{T_{1},text{coop}}, (95).
Finally, the outage probability of our system is: P_{text{out}} = P_{alpha}P_{text{out}}^{text{first-phase}}+ 1- P_{alpha})P_{text{out}}^{text{second-phase}} (25).
The outage probability in underlay approach (P_{text {out}}^{U,varepsilon }) (resp. interweave approach (P_{text {out}}^{I})) is given: P_{text{out}}^{U,varepsilon} = Prleft(C^{U}
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com