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Final report on link level and system level channel models - Winner

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WINNER D5.4 v. 1.4<br />

the ZDSC. The 10 rays are spaced in angle domain <strong>and</strong> have identical power. The power of each ray is<br />

P n /10, where P n is the average power of the nth ZDSC. The offset angle spacing depends <strong>on</strong> the value of<br />

AS of ZDSC_D for the departure side <strong>and</strong> value of AS of ZDSC_A for the arrival side. The AS<br />

<strong>and</strong><br />

φ<br />

AS are per ZDSC <strong>and</strong> are different from the<br />

ϕ<br />

φ<br />

ϕ<br />

σ <strong>and</strong>σ , respectively, which are the composite<br />

angle-spread involving all ZDSC. The rays of the ZDSC have r<strong>and</strong>om phases. The angle distributi<strong>on</strong>s <strong>and</strong><br />

power azimuth spectrum at the transmitter or receiver sides may vary from <strong>on</strong>e scenario to another. Table<br />

3.8 states the angle distributi<strong>on</strong>s of different scenarios that are defined in WINNER generic <strong>channel</strong><br />

model. The σ <strong>and</strong> σ influence in generati<strong>on</strong> of the ZDSC directi<strong>on</strong>al informati<strong>on</strong> through the<br />

φ<br />

ϕ<br />

parameters r<br />

φ <strong>and</strong>r ϕ , respectively. The locati<strong>on</strong> parameter for all distributi<strong>on</strong>s is zero <strong>and</strong> the scaling<br />

parameters are defined by r φ<br />

σ φ for departure angles <strong>and</strong> by r ϕ<br />

σ ϕ for arrival angles. The generati<strong>on</strong> of<br />

the angle offsets from the rays from cluster mean angle depends <strong>on</strong> AS<br />

φ for departure side <strong>and</strong> <strong>on</strong><br />

ASϕ<br />

arrival cluster. The offset angles are determined by multiplicati<strong>on</strong> of the angles spread per ZDSC<br />

with basis vector of offset angles (BO), e.g., AS<br />

φ *BO. Table 3.9 states the number of ZDSCs <strong>and</strong> the<br />

number of rays in each cluster as well as their AS<br />

φ <strong>and</strong> AS<br />

ϕ for the c<strong>on</strong>sidered scenarios. The angles<br />

of BO vector <strong>and</strong> the calculati<strong>on</strong> of the offset angles are presented in Table 3.10.<br />

ϕ<br />

φ<br />

Scenarios<br />

AoD<br />

distributi<strong>on</strong><br />

AoD<br />

scaling<br />

parameter<br />

AoA<br />

distributi<strong>on</strong><br />

AoA<br />

scaling<br />

parameter<br />

Table 3.8: Distributi<strong>on</strong>s of azimuth <strong>and</strong> departure angles.<br />

A1 B1 B3 C1 C2 D1<br />

LOS NLOS LOS NLOS LOS NLOS LOS NLOS NLOS LOS NLOS<br />

Wrapped Gaussian<br />

2.0σ φ 1.2σ φ 3.4σ φ 1.1σ φ 1.9σ φ 1.3σ φ 1.4σ ϕ 2.3σ φ 3.2σ φ 0.8σ ϕ 1.2σ<br />

φ<br />

Wrapped Gaussian<br />

1.7σ ϕ 2.1σ ϕ 3.6σ ϕ 3.6σ ϕ 1.5σ ϕ 1.6σ ϕ 1.8σ ϕ 1.8σ ϕ 3.2σ ϕ 2.2σ ϕ 1.3σ<br />

ϕ<br />

Scenarios<br />

Table 3.9: Number of ZDSCs <strong>and</strong> the number of rays in each cluster.<br />

A1 B1 B3 C1 C2 D1<br />

LOS NLOS LOS NLOS LOS NLOS LOS NLOS NLOS LOS NLOS<br />

Number of ZDSC 16 11 8 16 15 24 15 14 20 11 10<br />

Rays per ZDSC 10<br />

AS<br />

φ (deg) 5 5 3 10 4.7 5.5 5 2 2 1.5 1.5<br />

AS<br />

ϕ (deg) 5 5 18 22 5.4 12.5 5 10 15 3 3<br />

Table 3.10: Offset angles Rays within a ZDSC as a functi<strong>on</strong> of<br />

AS<br />

φ ,<br />

Ray number Basis vector offset angles (BO) Rays offset angles<br />

1,2 ± 0.0742<br />

3,4 ± 0.2532<br />

5,6 ± 0.4986<br />

7,8 ± 0.8913<br />

AS<br />

ϕ , AS ϕ , <strong>and</strong> AS θ .<br />

OA = AS X BO<br />

Page 24 (167)

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