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Exact(29)
Integrating the first equation of (1.4) over, we have (4.8).
Since, integrating the first inequality in the (2.12) from to, we have (2.13).
Integrating the first equation in the system (35) we get: F 1 = g 1 ζ, (36).
Integrating the first equation in (19) yields g = m 0 f + c 1, (20).
Integrating the first equation of system (2.1) over from to and over from to, respectively, we obtain (2.3).
Integrating the first two equations of (1.5) over and adding the results linearly, we have that, by Young inequality, (3.1).
Similar(31)
end{aligned}Integrating the first-order component the general solution begin{aligned} y=frac{displaystyle C_1^3}{displaystyle (C_1x+1)^2+C_1^2+1+C_2exp {(C_1x)}} end{aligned}of Eq. (17) follows.
On the contrary, our proposed algorithm alleviates two-hop rate mismatch by integrating the first-hop parameters and the timesharing value in relay transmit beamforming design, thus improving the end-to-end sum-rates.
end{array} end{aligned}Integrating the first-order component the general solution begin{aligned} y=big (1+C_1e^{-x}big )left( C_1^2displaystyle int frac{displaystyle dx}{displaystyle (C_1+e^x)^2}-log {big ( C_1+e^xbig )} -frac{small 1}{small 2}x^2+C_2right) +2x end{aligned}of (9) follows; this equation does not have any Lie symmetry.
Integrating the second equation of (2.16) along, we have.
Integrating the third equation of (2.16) along, we obtain.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com