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STAMATIOU et al.: SPATIAL MULTIPLEXING IN RANDOM WIRELESS NETWORKS 11<br />

Transm. cap. (nats/symbol/m 2 )<br />

0.0003<br />

0.00025<br />

0.0002<br />

0.00015<br />

N = 8<br />

0.0001<br />

5e-05<br />

N = 4<br />

DB, eq. (43)<br />

Sim, DB<br />

ZF, eq. (32)<br />

Sim, ZF<br />

VB, eq. (36)<br />

Sim, VB<br />

0<br />

1 2 3 4 5 6 7 8<br />

Fig. 4. Transmission capacity vs. M for N = 4, 8 (ǫ = 0.1, R = 20 m,<br />

b = 3, θ = 6 dB). The optimal number of streams for DBLAST is 3 when<br />

N = 4, <strong>and</strong> 6 when N = 8. These numbers are <strong>in</strong> accordance with (45). In<br />

the case of ZF, the optimal number of streams is 1 when N = 4, <strong>and</strong> 3 when<br />

N = 8. These numbers are also <strong>in</strong> accordance with (35). To avoid clutter<strong>in</strong>g<br />

the figure, DBLAST is denoted as DB <strong>and</strong> VBLAST as VB.<br />

Transm. cap. (nats/symbol/m 2 )<br />

0.0004<br />

0.00035<br />

0.0003<br />

0.00025<br />

0.0002<br />

M<br />

N = 8<br />

0.00015<br />

0.0001<br />

5e-05<br />

N = 4<br />

DB, eq. (43)<br />

Sim, DB<br />

ZF, eq. (32)<br />

Sim, ZF<br />

VB, eq. (36)<br />

Sim, VB<br />

1 2 3 4 5 6 7 8<br />

Fig. 5. Transmission capacity vs. M for N = 4, 8 (ǫ = 0.1, R = 20 m,<br />

b = 4, θ = 6 dB). To avoid clutter<strong>in</strong>g the figure, DBLAST is denoted as DB<br />

<strong>and</strong> VBLAST as VB.<br />

In Fig. 3, the theoretical <strong>and</strong> simulated success probability<br />

of ZF <strong>and</strong> DBLAST are plotted vs. the density of the PPP for<br />

a system where M = 3 antennas are employed <strong>in</strong> each TX.<br />

The agreement between theory <strong>and</strong> simulation is once aga<strong>in</strong><br />

very satisfactory, which, <strong>in</strong> the case of DBLAST, confirms the<br />

validity of the approximations <strong>in</strong> Section IV-C.<br />

Fig. 4 shows the dependence of the transmission capacity<br />

on the number of transmitted streams for the three MIMO<br />

techniques considered <strong>in</strong> Section IV. The total number of<br />

antennas takes two values N = 4, 8, the propagation exponent<br />

is b = 3 <strong>and</strong> a constra<strong>in</strong>t ǫ = 0.1 is placed on the outage<br />

probability. The DBLAST transmission scheme results <strong>in</strong><br />

higher transmission capacity compared to VBLAST or simple<br />

ZF. Moreover, the ga<strong>in</strong> between VBLAST <strong>and</strong> simple ZF is<br />

marg<strong>in</strong>al, which is attributed to the fact that, with VBLAST,<br />

the maximum contention density is still determ<strong>in</strong>ed by the<br />

sub<strong>channel</strong> with the smallest diversity order.<br />

M<br />

Transm. cap. (nats/symbol/m 2 )<br />

4e-05<br />

3.5e-05<br />

3e-05<br />

2.5e-05<br />

2e-05<br />

1.5e-05<br />

1e-05<br />

5e-06<br />

DBLAST<br />

Sim, DBLAST<br />

ZF<br />

Sim, ZF<br />

ZF, M = N<br />

Sim, ZF, M = N<br />

MRC<br />

Sim, MRC<br />

0<br />

1 2 3 4 5 6 7 8<br />

Fig. 6. Transmission capacity vs. N (ǫ = 0.01, R = 20 m, b = 4,<br />

θ = 6 dB). If all TX antennas are activated, the transmission capacity of ZF<br />

is lower than the transmission capacity of MRC, even though the scal<strong>in</strong>g <strong>in</strong><br />

both cases is Θ( √ N). Sett<strong>in</strong>g M = N <strong>and</strong> b = 4 <strong>in</strong> (32) we can also see<br />

that TCzf TCǫ<br />

ǫ ≈ , which is confirmed by the plot.<br />

Γ(1/2)<br />

Optimal M<br />

8<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

DBLAST<br />

ZF<br />

1 2 3 4 5 6 7 8<br />

N<br />

Fig. 7. Optimal number of streams vs. N (ǫ = 0.01, R = 20 m, b = 4,<br />

θ = 6 dB).<br />

In Fig. 5, the propagation exponent takes the value b = 4.<br />

As predicted <strong>in</strong> Section IV-C, activat<strong>in</strong>g all the TX antennas<br />

maximizes the transmission capacity for DBLAST. In the case<br />

of ZF, the optimal number of streams is dictated by (35).<br />

Overall, <strong>in</strong> both Fig. 4 <strong>and</strong> Fig. 5, the agreement between<br />

theory <strong>and</strong> simulation is satisfactory.<br />

In Fig. 6 <strong>and</strong> Fig. 7, the transmission capacity <strong>and</strong> the<br />

respective - optimal - number of streams are plotted vs. N for<br />

DBLAST, ZF <strong>and</strong> MRC <strong>and</strong> an outage probability constra<strong>in</strong>t<br />

ǫ = 0.01. As predicted <strong>in</strong> Section IV, <strong>in</strong> the case of DBLAST<br />

<strong>and</strong> ZF, <strong>and</strong> optimally selected M, the transmission capacity<br />

scales l<strong>in</strong>early <strong>in</strong> N, while, <strong>in</strong> the case of MRC, it scales as<br />

N α = √ N. At N ≥ 3, DBLAST provides a capacity ga<strong>in</strong> of<br />

approximately 1.4 compared to ZF, which is <strong>in</strong> agreement with<br />

the √ 2 ga<strong>in</strong> predicted at the end of Section IV-C. Moreover,<br />

it is observed that, for N ≤ 3, MRC <strong>and</strong> ZF result <strong>in</strong><br />

approximately the same transmission capacity.<br />

N

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