Resource Allocation in OFDM Based Wireless Relay Networks ...
Resource Allocation in OFDM Based Wireless Relay Networks ...
Resource Allocation in OFDM Based Wireless Relay Networks ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
4.3 Cooperative Non-Orthogonal Transmission<br />
The optimization can be stated as<br />
max<br />
π,p,w<br />
C , s.t. (4.5), (4.6), (4.4), (4.7)<br />
with π = {π (k,j) }, p = {p k }, w = {w n,j }, and p k ≥ 0, w n,j ≥ 0, for all n =<br />
{1, ..., N}, k = {1, ..., K}, j = {1, ..., K}.<br />
4.3.1 Jo<strong>in</strong>t Optimization Algorithm<br />
F<strong>in</strong>d<strong>in</strong>g the power variables p k and the beamform<strong>in</strong>g weights w n,j together seems<br />
difficult.<br />
Fortunately, the structure of the problem permits to first compute the<br />
optimal beamform<strong>in</strong>g coefficients for a given source power p k . Denote ρ j as the<br />
total power allocated to sub-carrier j such that ∑ K<br />
j=1 ρ j ≤ P R . Then (4.7) can be<br />
re-stated as<br />
max<br />
π,p,w C (4.8)<br />
s.t.<br />
K∑ K∑ ∑ N K∑<br />
|w n,j | 2 (p k |h n,k | 2 + σr) 2 ≤ ρ j ,<br />
k=1 j=1<br />
π (k,j)<br />
n=1<br />
K∑<br />
ρ j ≤ P R , (4.6), (4.4).<br />
j=1<br />
Thus, for any sub-carrier pair (k, j) with known p k<br />
problem can be stated as<br />
max<br />
w<br />
s.t.<br />
j=1<br />
the optimum beamform<strong>in</strong>g<br />
log 2 (1 + SNR (k,j) ) (4.9)<br />
N∑<br />
|w n,j | 2 (p k |h n,k | 2 + σr) 2 ≤ ρ j . (4.10)<br />
n=1<br />
S<strong>in</strong>ce the logarithm is a monotonically <strong>in</strong>creas<strong>in</strong>g function, maximization of the<br />
objective <strong>in</strong> (4.9) is equivalent to the maximization of (4.2). Def<strong>in</strong><strong>in</strong>g<br />
√<br />
γn,k γ n,j<br />
ψ = , ξ = 1 + γ n,k + γ n,j<br />
. (4.11)<br />
1 + γ n,j 1 + γ n,k<br />
with<br />
γ n,k = |h n,k| 2 p k<br />
σ 2 r<br />
, andγ n,j = |g n,j| 2 ρ j<br />
,<br />
σd<br />
2<br />
66