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The effective received signal after interference cancelation can be represented as Y = X ⋅ H + I + W. (30).
This means that h(t) is proportional to the effective received waveform w(t) and, consequently, the performance of the IMF can be obtained by setting ρ = 1 in (23).
Since is independent of, the destination can perfectly cancel from its received signal, and thus, from (7), the effective received signal at the destination can be written as (49).
Note that the effective received signal at the BSA output is in the time-multiplexed form of the BSA input signals y u as illustrated in Fig. 3. Fig. 3 Example of received signal at the BSA with M R=4 and Ω=2.
Thus, the effective received signal vector at the kth receiving node is given by {begin{aligned} mathbf{y}_{k}=mathbf{H}_{k}^{T} mathbf{F}mathbf{H}_{bar {k}}mathbf{B}_{bar{k}}mathbf{s}_{bar{k}} + mathbf{H}_{k}^{T}mathbf{F} left(sum_{jneq k,{bar{k}}}^{2K}mathbf{H}_{j}mathbf{B}_{j}mathbf{s}_{j} + mathbf{n}_{mathrm{r}}right) + mathbf{n}_{mathrm{d},k}, end{aligned}} (35).
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Similar(54)
Assuming that the distance between the transmitter and receiver is much greater than the effective receiving area of the detector, the received power at the detector is approximately a constant over the surface of the receiver.
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It is shown that adequate knowledge of effective receive subspaces can be attained by simply assuming matched filters (MF) in the iterative precoding process, while further improvement can be obtained by an actual implementation of interference-mitigation-capable receivers.
More precisely, only a small part of the effective receive signal termination is provided by an external resistor, while the main part is actively generated by the LD itself.
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