Final report on link level and system level channel models - Winner
Final report on link level and system level channel models - Winner
Final report on link level and system level channel models - Winner
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WINNER D5.4 v. 1.4<br />
• Cross-polarizati<strong>on</strong> ratio (XPR). No distincti<strong>on</strong> is made between clusters <strong>and</strong> segments in the<br />
current model. Therefore, the resulting variability of XPR is equivalent if evaluated across<br />
clusters or across segments.<br />
• Total angle-spread <strong>and</strong> delay-spread. These parameters characterize the power dispersi<strong>on</strong> in<br />
angle <strong>and</strong> delay domain across clusters. Note that this is a high-<strong>level</strong> characterizati<strong>on</strong>. The more<br />
detailed properties of angle <strong>and</strong> delay dispersi<strong>on</strong> are each defined by a set of two variables. This<br />
is firstly, a mean angle <strong>and</strong> a delay offset for each single cluster, <strong>and</strong> sec<strong>on</strong>dly, an angle-spread<br />
<strong>and</strong> a delay-spread for each cluster. Here,<br />
• The angle-spread per cluster <strong>and</strong> delay-spread per cluster values are c<strong>on</strong>stants.<br />
• The mean angle per cluster <strong>and</strong> the delay offset per cluster distributi<strong>on</strong>s are functi<strong>on</strong>s of<br />
the total (per segment) angle-spread <strong>and</strong> the total (per segment) delay-spread.<br />
Large-scale parameters of the <strong>channel</strong> have clear influence <strong>on</strong> the <strong>channel</strong> characteristics. This can be<br />
noticed in delay domain characteristics through the RMS delay spread <strong>and</strong> in the angle domain through<br />
the RMS angle-spread in departure <strong>and</strong> in arrival. The RMS delay spread has influence <strong>on</strong> power delay<br />
spectrum <strong>and</strong> <strong>on</strong> the probability density functi<strong>on</strong> (pdf) of path delays through the parameter r τ .. The<br />
statistical distributi<strong>on</strong>s that generate spatial properties of the ZDSCs are functi<strong>on</strong>s of RMS angle-spread<br />
through azimuth angle propati<strong>on</strong>ality factor ( r ϕ ) <strong>and</strong> RMS azimuth angle-spread ( σ ϕ ) in the arrival side,<br />
<strong>and</strong> through departure angle proporti<strong>on</strong>ality factor ( r φ ) <strong>and</strong> RMS departure angle-spread ( σ φ ) in the<br />
departure side. The dispersi<strong>on</strong> parameters σ ϕ <strong>and</strong> σ φ are sometimes correlated with log-normal<br />
shadowing (LNS), which is important for interference calculati<strong>on</strong>s, h<strong>and</strong>over algorithms, etc. For each set<br />
of RMS delay spread <strong>and</strong> RMS angle-spread departure, RMS angle-spread departure arrival <strong>and</strong> LNS<br />
within each <strong>channel</strong> segment, correlati<strong>on</strong> between them has to be c<strong>on</strong>sidered. These large-scale<br />
parameters are often <str<strong>on</strong>g>report</str<strong>on</strong>g>ed in literature to have log-normal distributi<strong>on</strong>s.<br />
Our framework allows for any distributi<strong>on</strong> for the large-scale parameters <strong>and</strong> also introduces a modelling<br />
of the auto-correlati<strong>on</strong> over the service area. This is achieved by using scenario <strong>and</strong> parameter specific<br />
g ⋅ to transform the large-scale parameters into a domain where they can be treated as<br />
transformati<strong>on</strong>s ( )<br />
Gaussian. The mean, µ , cross-correlati<strong>on</strong> <strong>and</strong> auto-correlati<strong>on</strong> matrix R ( 0)<br />
are then defined in the<br />
transformed domain. The realizati<strong>on</strong>s of the large-scale parameters are then obtained as<br />
−1<br />
0.5<br />
−1<br />
0.5<br />
0.5<br />
5<br />
g R ? x, y + µ<br />
⋅<br />
R 0 is obtained as R ( 0) = EΛ<br />
0.<br />
( ( ) ), where g ( ) is the inverse transform, <strong>and</strong> ( )<br />
T<br />
from the eigen-decompositi<strong>on</strong> R( 0 ) = EΛE<br />
of R ( 0)<br />
. The auto-correlati<strong>on</strong> is achieved by generating m<br />
( m = 6 for A1, <strong>and</strong> m = 4 for all other scenarios) independent Gaussian r<strong>and</strong>om processes,<br />
? x, y = ξ1 x,<br />
y Kξ<br />
m<br />
x,<br />
y , each <strong>on</strong>e with mean zero <strong>and</strong> variance <strong>on</strong>e in the positi<strong>on</strong>s x, y where the<br />
( ) [ ( ) ( )] T<br />
mobiles are located. The auto-correlati<strong>on</strong> of the process c<br />
( x,<br />
y)<br />
2<br />
E{ ξ ( x y ) ξ ( x , y )} = exp( − r / λ ), where ( ) ( ) 2<br />
c<br />
1, 1 c 2 2<br />
∆<br />
c<br />
∆ r =<br />
no auto-correlati<strong>on</strong> mode (NACM) in which the parameters<br />
the r<strong>and</strong>om variable ?( x, y) [ ξ ( x,<br />
y) ( x y)<br />
] T<br />
1<br />
Kξ<br />
m<br />
,<br />
x<br />
1 − x0<br />
+ y1<br />
− y0<br />
m<br />
ξ is given by<br />
. However, we also define a<br />
λ , K ,λ are all set to zero, or equivalently,<br />
= , is r<strong>and</strong>omized independently for each locati<strong>on</strong>. The<br />
required parameters for generating the correlated large-scale parameters are thus the transformati<strong>on</strong><br />
~<br />
s ( x , y)<br />
= g( s( x,<br />
y)<br />
) (or actually its inverse), the mean µ <strong>and</strong> correlati<strong>on</strong> R ( 0)<br />
of the transformed largescale<br />
parameters, <strong>and</strong> the de-correlati<strong>on</strong> distance parameters λ , K 1<br />
,λm<br />
.<br />
This informati<strong>on</strong> is available in Table 3.1 to Table 3.5. Table 3.1 lists the distributi<strong>on</strong> functi<strong>on</strong> for each<br />
modelled parameter in each scenario. For normally distributed r<strong>and</strong>om variables the original <strong>and</strong><br />
transformed variable is identical, except for the delay-spread in scenario B3, where the transformati<strong>on</strong> is a<br />
9<br />
multiplicati<strong>on</strong> with a factor 10 (for numerical reas<strong>on</strong>s). For parameters of log-Gumbel <strong>and</strong> log-Logistic<br />
distributi<strong>on</strong>, the transformati<strong>on</strong> (<strong>and</strong> their inverse) are given by:<br />
~<br />
−<br />
s = g s = −Q<br />
1 F log s ,ν ,ς<br />
(3.1)<br />
<strong>and</strong><br />
( ) (<br />
Gumbel( 10<br />
( ) ))<br />
−1<br />
( ~ −1<br />
s = g s ) = exp log(10) F Q(<br />
~ s ),ν ,ς<br />
Gumbel<br />
−<br />
1<br />
( ( ))<br />
1 ( F Logistic 10<br />
)<br />
−1<br />
( log(10) F ( Q(<br />
~ s ),ν ,ς ))<br />
−<br />
( s) = −Q<br />
( log ( s)<br />
,ν ,ς )<br />
(3.2)<br />
~<br />
s = g<br />
, (3.3)<br />
−1<br />
s = g ( ~ s ) = exp<br />
Logistic<br />
−<br />
(3.4)<br />
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