modelling and simulation of mimo channels
TRANSCRIPT
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Modelling and Simulation of MIMO Channels
Matthias Pätzold
Agder University College
Mobile Communications Group
Grooseveien 36, NO-4876 Grimstad, Norway
E-mail: [email protected]: http://ikt.hia.no/mobilecommunications/
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Contents
I. Introduction
II. Principles of Fading Channel Modelling
III. Modelling of MIMO Channels
IV. Simulation of MIMO Channels
V. Conclusion
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I. Introduction
Mobile Communications Using Smart Antennas
Realistic spatio-temporal channel models are required for the design, test, and optimization
of mobile communication systems employing smart antenna technologies.
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Meaning of Channel Modelling and Simulation for Mobile Communications
Reference system:
+Channelmodel
Noise
Data source Data sink
Transmitter Receiverd(i) x(t) y(t) d̂(i)
⇒ Performance measure: Bit error probability P b = f
E bN 0
Simulation system:
+Channel
Noise
Data source Data sink
Transmitter Receiversimulator
d(i) x(t) ỹ(t) d̃(i)
⇒ Performance measure: Bit error probability P̃ b = f
E bN 0
, ∆β
≈ P b
↑Model error• The model error ∆β describes the essential error which is introduced by the channel simulator.
Channel simulators are important for the test, the parameter optimization, and the perfor-
mance analysis of mobile communication systems.
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The Two Main Categories of Fading Channel Simulators
Simulators based on reference models: Simulators based on measurements:
Simulation model
Reference model
Measurement
Real-world
Snapshotmeasurementscampaigns
channel channelReal-world
Simulation model
Problem: Reference models are not
close to real-world channels.
Problem: Finding of typical scenarios.
⇒ The dilemma of mobile fading channel modelling.
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Some Requirements for Fading Channel Simulators
• High precision w.r.t. a given reference model or w.r.t. measured channels
• High efficiency
• The underlying stochastic channel simulator must be ergodic to reduce the number of trials
• Easy to determine the model parameters
• Easy to understand and easy to implement
• Reproducibility for enabling fair performance comparisons
• Easy to extend (frequency selectivity, spatial selectivity, multi-cluster propagation scenarios, numberof antenna elements, etc.)
• Low complexity
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II. Principles of Fading Channel Modelling
Two Fundamental Methods for Modelling of Coloured Gaussian Noise Processes
1. Filter method:
⇒ Stochastic process µ(t)
⇒Reference model
2. Sum-of-sinusoids (SOS) method:
cos(2πf 1t + θ1)
cos(2πf 2t + θ2)
cos(2πf N t + θN )
c1
c2
cN ...
...
... ...∞ ∞
⊗ ⊗
⊗ + µ(t)
⇒ Stochastic process µ(t)⇒ Reference model
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For a finite number of harmonic functions N , we obtain:
Parameters: ensemble
θn = Random variable (RV)
f n = const.
cn = const.
cos(2πf 1t + θ1)
cos(2πf 2t + θ2)
cos(2πf N t + θN )
c1
c2
cN ... ...
⊗ ⊗
⊗
+ µ̂(t)
⇒ Stochastic process µ̂(t)⇒ Stochastic simulation model
Parameters: single realization
θn = const.
f n = const.
cn = const.
cos(2πf 1t + θ1)
cos(2πf 2t + θ2)
cos(2πf N t + θN )
c1
c2
cN ...
...
⊗ ⊗
⊗ + µ̃(t)
⇒ Deterministic process µ̃(t)⇒ Deterministic simulation model
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Relationships Between Stochastic Processes, Random Variables,Sample Functions, and Real-Valued Numbers
Gaussian process: µ(t) = limN →∞
N n=1
cn cos(2πf nt + θn) (cn = const., f n = const., θn = RV)
Stochastic process: µ̂(t) =N
n=1
cn cos(2πf nt + θn) (cn = const., f n = const., θn = RV)
simulationmodel
Deterministic
Stochasticsimulationmodel
modelReference
Gaussian process
Stochastic process
Random
variable
Sample
function
Real number
t = t0
θn = const. t = t0
µ̂(t0) = µ̂(t0, θn)
µ̂(t0) = µ̃(t0)
µ̃(t) = µ̂(t, θn)
N < ∞N → ∞
µ̂(t) = µ̂(t, θn)
µ(t) = µ(t, θn)
θn = const.
θn = RV
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Principle of Deterministic Channel Modelling
Step 1: Starting point is a reference model derived from one, two or several Gaussianprocesses.
Step 2: Derive a stochastic simulation model from the reference model by replacing eachGaussian process by a sum-of-sinusoids with fixed gains, fixed frequencies, and
random phases.
Step 3: Determine the deterministic simulation model by fixing all model parameters of thestochastic simulation model, including the phases.
Step 4: Compute the model parameters of the simulation model by using a proper param-eter computation method.
Step 5: Simulate one (or some few) sample functions (deterministic processes).
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Example: Derivation of a channel simulator for Rice processes
Step 1: Reference model Steps 2 & 3: Simulation model
ρµ (t)
(t)µ2
1(t)µ
πf t+θm (t)= ρ ρ)ρ2 sin(2
cos(2 πf t+θm (t)=1 ρ ρ)ρ
H (f)
H (f)
(t)2v
(t)1v
ξ(t)
ρµ
ρµ (t)
(t)
WGN
WGN
2
1
⇐⇒
⇒Stochastic Rice process ξ (t)
⇒Deterministic Rice process ξ̃ (t)
Step 4: Compute the model parameters by fitting the statistics of the deterministic simulationmodel to those of the stochastic reference model.
Step 5: Simulate the deterministic Rice process ξ̃ (t).
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Methods for the Calculation of the Model Parameters
Deterministic process: µ̃i(t) =
N in=1
ci,n cos(2πf i,nt + θi,n)
↑ Model parameters: gains frequencies phases
Historical overview
Methods Disadvantages
Rice method (Rice, 1944) Small period
Jakes method (Jakes, 1974) Special case only
Monte Carlo method (Schulze, 1988) Non-ergodic
Method of equal distances (Pätzold, 1994) Small period
Method of equal areas (Pätzold, 1994) Slow convergency
Harmonic decomposition technique (Crespo, 1995) Small period
Mean-square-error method (Pätzold, 1996) Small period
Method of exact Doppler spread (Pätzold, 1996) Special case only
L p-norm method (Pätzold, 1996) –
Method porposed by Zheng and Xiao (2002) Non-ergodic
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Classes of SOS Channel Simulators and Their Statistical Properties
Deterministic process: µ̃i(t) =N i
n=1ci,n cos(2πf i,nt + θi,n)
Class Gains Frequencies Phases First-order Wide-sense Mean- Autocor.-
ci,n f i,n θi,n stationary stationary ergodic ergodic
I const. const. const. – – – –
II const. const. RV yes yes yes yes
III const. RV const. no/yes a no/yes a no/ yes a no
IV const. RV RV yes yes yes no
V RV const. const. no no no/yes a no
VI RV const. RV yes yes yes no
VII RV RV const. no/yes a no/yes a no/yes a no
VIII RV RV RV yes yes yes no
a
If certain boundary conditions are fulfilled.
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Application of the Scheme to Parameter Computation Methods
Stochastic process: µ̂i(t) =N in=1
ci,n cos(2πf i,nt + θi,n)
↑ Model parameters: gains frequencies phases (RVs)
Parameter computation methods Class FOS WSS Mean-ergodic Autocor.-ergodic
Rice method II yes yes yes yes
Monte Carlo method IV yes yes yes no
Jakes method II yes yes yes yesHarmonic decomposition technique II yes yes yes yes
Method of equal distances II yes yes yes yes
Method of equal areas II yes yes yes yes
Mean-square-error method II yes yes yes yes
Method of exact Doppler spread II yes yes yes yes
L p-norm method II yes yes yes yes
Method proposed by Zheng and Xiao IV yes yes yes no
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Applications of the Principle of Deterministic Channel Modelling
• Frequency-nonselective channels (Rayleigh, Rice, ext. Suzuki, Nakagami, etc.),
• Frequency-selective channels (COST 207, CODIT),
• Space-time wideband channels (COST 259),• Multiple cross-correlated Rayleigh fading channels,
• Multiple uncorrelated Rayleigh fading channels,
• Perfect modelling and simulation of measured 2-D and 3-D channels,
• Frequency-hopping fading channels,
• Design of ultra fast channel simulators (tables system),
• Design of burst error models,
• Development of MIMO channels.
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III. Modelling of MIMO Channels
Block Diagram of a MIMO Mobile Communication System
Transmitter Receiver
x1
x2
xM T
r1
r2
rM R
h11
h 1 2
h 2 1 h
M R
1
h22h M
R 2
h 1 M
T
hM RM T h 2
M T
•
•
•
•
•
•
•
•
•
•
•
•
• Channel coefficients: The channel coefficient hij(t) describes the transmission behavior of thechannel from the jth transmit antenna to the ith receive antenna.
• Channel matrix: H(t) = [hij(t)] ∈ CM R×M T
• Channel capacity: C (t) = log2 det
IM T + S BS, totalM T N noise
H(t)HH (t)
[bits/s/Hz]
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Generalized Principle of Deterministic Channel Modelling
Step 1: Starting point is a geometrical model with an infinite number of scatterers, e.g.,
(a) one-ring model (b) two-ring model (c) elliptical model
BS MS BS MS BS MS
Step 2: Derive a stochastic reference model from the geometrical model.
Step 3: Derive an ergodic stochastic simulation model from the reference model by usingonly a finite number of N scatterers.
Step 4: Determine the deterministic simulation model by fixing all model parameters of thestochastic simulation model.
Step 5: Compute the parameters of the simulation model by using a proper parametercomputation method, e.g., the L p-norm method (LPNM).
Step 6: Generate one (or some few) sample functions by using the deterministic simulationmodel with fixed parameters.
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Illustration of the Generalized Principle of Deterministic Channel Modelling
3 4 6
5
21
Infinite complexity
(N → ∞)
⇒ ⇒sample functions sample functions
Non-realizable Realizable⇒sample functions
Non-realizable
Reference model
E{·} E{·} < · >Statistical properties
Deterministic SoSsimulation model
computation
Parameter
Simulation of sample functions
Fixedparameters
Stochastic SoSsimulation model
Finite complexity
One (or some few)Infinite number of Infinite number of
Finite complexity
(N ≈ 25) (N ≈ 25)
Lp-norm method (LPNM)
Geometrical model
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Application of the Generalized Principle of Deterministic Channel Modelling
A Geometrical Model for a MIMO Channel
Dn2
Dn1A
BS
1
δBS
A2
MS
αMS
δMS
0MS
BSα
nBSφ
AMS
1
D2n
BSφmax
Sn
v
y
0BS
D
2ABS
φMSD
n
1n
x
R
v
α
• The geometrical model is known as the one-ring model for a 2 × 2 channel.• The local scatterers are laying on a ring around the MS.• If the number of scatterers N → ∞, then the discrete AOA φMSn tends to a continuous RV φ MS with
a given distribution p(φ MS), e.g., the uniform distribution, the von Mises distribution, the Laplacian
distribution, etc.
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The Reference Model
• Channel coefficients: h11(t) = limN →∞1
√ N N
n=1 anbne j(2πf nt+θn)
h12(t) = limN →∞
1√ N
N n=1
a∗nbne j(2πf nt+θn)
h21(t) = limN →∞
1
√ N
N
n=1
anb∗ne
j(2πf nt+θn)
h22(t) = limN →∞
1√ N
N n=1
a∗nb∗ne
j(2πf nt+θn)
where the phases θn are i.i.d. RVs and
an = e jπ(δ BS/λ)
[cos(α
BS )+φBS
max sin(α
BS )sin(φMS
n )
]
bn = e jπ(δ MS/λ)cos(φ
MS n −αMS )
f n = f max cos(φMSn − αv)
• Channel matrix: H(t) = [hij(t)] =
h11(t) h12(t)h21(t) h22(t)
• Channel capacity: C (t) = log2 det
I2 + S BS, total
2N noiseH(t)HH (t)
[bits/s/Hz]
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Statistical Properties of the Reference Model
• Space-time CCF: ρ11,22(δ BS, δ MS, τ ) := E {h11(t)h∗22(t + τ )}= lim
N →∞1
N
N n=1
a2n b2ne
− j2πf nτ
=
π
−π a
2
n(δ BS)b
2
n(δ MS)e − j2πf nτ
p(φ
MS
)dφ
MS
• Time ACF: rh11(τ ) := E {h11(t)h∗11(t + τ )}
=
π −π
e − j2πf max cos(φMS−αv)τ p(φMS) dφMS
Relationships: rh11(τ ) = rh12(τ ) = rh21(τ ) = rh22(τ ) = ρ11,22(0, 0, τ )
• 2D space CCF: ρ(δ BS, δ MS) := ρ11,22(δ BS, δ MS, 0)
=
π −π
a2n(δ BS)b2n(δ MS) p(φ
MS)dφMS
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The Stochastic Simulation Model
• Channel coefficients: ĥ11(t) = 1√ N
N n=1
anbne j(2πf nt+θn)
⇒ The phases θn are i.i.d. RVs
• Channel matrix: Ĥ(t) =
ĥ11(t) ĥ12(t)
ĥ21(t) ĥ22(t)
⇒ Stochastic channel matrix
• Channel capacity: Ĉ (t) = log2 det
I2 + S BS, total
2N noiseĤ(t) ĤH (t)
[bits/s/Hz]
⇒ Stochastic process
⇒ The analysis of Ĉ (t) has to be performed by using statistical aver-ages, e.g., C s = E {Ĉ (t)}.
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Statistical Properties of the Stochastic Simulation Model
• Space-time CCF: ρ̂11,22(δ BS, δ MS, τ ) : = E
{ĥ11(t)ĥ
∗22(t + τ )
}=
1
N
N n=1
a2n(δ BS)b2n(δ MS)e
− j2πf nτ
• Time ACF: r̂h11(τ ) : = E
{ĥ11(t)ĥ
∗11(t + τ )
}=
1
N
N n=1
e − j2πf max cos(φMS
n −αv)τ
Relationships: r̂h11(τ ) = r̂h12(τ ) = r̂h21(τ ) = r̂h22(τ ) = ρ̂11,22(0, 0, τ )
• 2D space CCF: ρ̂(δ BS, δ MS) : = ρ̂11,22(δ BS, δ MS, 0)
= 1
N
N
n=1
a2n(δ BS)b2n(δ MS)
= 1
N
N n=1
e j2π(δ BS/λ)[cos(αBS)+φBS
max sin(αBS)sin(φMS
n )]·e j2π(δ MS/λ)cos(φMSn −αMS)
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The Deterministic Simulation Model
• Channel coefficients: h̃11(t) = 1√ N
N n=1
anbne j(2πf nt+θn)
⇒ The phases θn are constant quantities
• Channel matrix: H̃(t) =
h̃11(t) h̃12(t)
h̃21(t) h̃22(t)
⇒ Deterministic channel matrix
• Channel capacity: C̃ (t) = log2 det
I2 + S BS, total
2N noiseH̃(t) H̃H (t)
[bits/s/Hz]
⇒ Deterministic process
⇒ The analysis of C̃ (t) has to be performed by using time averages,e.g., C t =< C̃ (t) >.
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Statistical Properties of the Deterministic Simulation Model
• Space-time CCF: ρ̃11,22(δ BS, δ MS, τ ) :=
= 1
N
N n=1
a2n(δ BS)b2n(δ MS)e
− j2πf nτ
• Time ACF: r̃h11(τ ) := <
h̃11(t)h̃∗11(t + τ ) >
= 1
N
N n=1
e − j2πf max cos(φMS
n −αv)τ
Relationships: r̃h11(τ ) = r̃h12(τ ) = r̃h21(τ ) = r̃h22(τ ) = ρ̃11,22(0, 0, τ )
• 2D space CCF: ρ̃(δ BS, δ MS) : = ρ̃11,22(δ BS, δ MS, 0)
= 1
N
N
n=1
a2n(δ BS)b2n(δ MS)
= 1
N
N n=1
e j2π(δ BS/λ)[cos(αBS)+φBS
max sin(αBS)sin(φMS
n )]·e j2π(δ MS/λ)cos(φMSn −αMS)
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Parameter Computation Method
Parameters: The model parameters to be determined are the discrete AOAs φMSn (n = 1, 2, . . . , N ).
Aim: Determine the model parameters φMSn such that
ρ11,22(δ BS, δ MS, τ ) ≈ ρ̃11,22(δ BS, δ MS, τ ) .
Solution: L p-norm method
E ( p)1 :=
1τ max
τ max 0
|rh11(τ ) − r̃h11(τ )| pdτ 1/p
E ( p)2 :=
1δ BSmax δ
MSmax
δ BSmax 0
δ MSmax 0
|ρ(δ BS, δ MS) − ρ̃(δ BS, δ MS)| pdδ MS dδ BS1/p
Two alternatives: (i) Joint optimization: E ( p) = w1E ( p)1 + w2E
( p)2
w1, w2: weighting factors
(ii) Using two independent sets {φMSn } and {φMSn }in r̃h11(τ ) and ρ̃(δ BS, δ MS), respectively.
⇒ Orthogonalization of the optimization problem.
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Structure of the Simulation Model
+
. . .
. . .
. . .
. . . . . .
. . .
. . .
. . .
. . .. . .
. . .
.
.
.
.
.
.
+
.
.
.
.
.
.
1/√ N
1/√ N
1/√ N
s2(t)
r1(t) r2(t)
bN ∗b∗
2b∗1bN b2b1
a1 a2 aN
s1(t)
a∗N
a∗2
a∗1
e j(2πf N t + θN )
e j(2πf 2t + θ2)
e j(2πf 1t + θ1)
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Performance Evaluation
• Comparison of the time ACFs rh11(τ ) (reference model) and r̃h11(τ ) (simulation model)
0 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08 0.09 0.1−0.5
0
0.5
1
Time separation, τ (s)
T i m e
a u t o c o r r e l a t i o n f u n c t i o n
Reference modelSimulation modelSimulation
τmax
Reference model: Based on the one-ring model with uniformly distributed AOAs φMS.
Simulation model: Designed by using the L p-norm method (N = 25 , p = 2, τ max = 0.08 s, f max = 91 Hz).
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Reference model Simulation model
2-D space CCF ρ(δ BS, δ MS) 2-D space CCF ̃ρ(δ BS, δ MS)
0
5
10
15
20
25
30
0
0.5
1
1.5
2
2.5
3
−0.5
0
0.5
1
2 −
D
s p a c e c r o s s − c o r r e l a t i o n f u n c t i o n
0
5
10
15
20
25
30
0
0.5
1
1.5
2
2.5
3
−0.5
0
0.5
1
2 −
D
s p a c e c r o s s − c o r r e l a t i o n f u n c t i o n
δ MS/λ δ BS/λ δ MS/λ δ BS/λ
Reference model: Based on the one-ring model with uniformly distributed AOAs φMS.
Simulation model: Designed by using the Lp-norm method with N = 25
( p = 2, δ BSmax = 30λ, δ MSmax = 3λ, αBS = αMS = 90
◦, φBSmax = 2◦).
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IV. Simulation of MIMO Channels
• Channel capacity: C̃ (t) := log2 det
I2 + S BS, total
2N noiseH̃(t) H̃H (t)
[bits/s/Hz]
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.50
1
2
3
4
5
6
7
8
9
10
11
Time, t (s)
S i m u l a t e d c h a n
n e l c a p a c i t y ,
( b i t s / s / H z )
CapacityMean Capacity
Parameters: N = 25, M BS = M MS = 2, δ BS = δ MS = λ/2, SNR = 17 dB
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Scattering Scenario
Geometrical one-ring model:
scatterersCluster of
δ BS
y
xδ MS
αvφBSmaxv
≈ 2√ κ
Parameters:
M BS = M MS = 2
δ BS = δ MS = λ/2φBSmax = 2
◦
αv = φMS0 = 180
◦
f max = 91 Hz
Reference model: assuming the von Mises distribution for the AOA φMS :
p(φMS) = 1
2πI 0(κ)
e κ cos(φMS−φMS0 )
κ = 0 : p(φMS) = 1/(2π) (isotropic scattering)
κ → ∞ : p(φMS) → δ (φMS − φMS0 ) (extremely nonisotropic scattering)Simulation model: designed by using the LPNM with N = 25.
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Normalized ADF of the Channel Capacity C̃(t)
0 2 4 6 8 100
50
100
150
200
250
300
350
400
450
500
Level, r
T C
( r ) ⋅ f m
a x
κ = 0
κ = 10
κ = 100
Observations: • κ has a strong influence on the ADF T̃ C (r) of the capacity C̃ (t)• If κ ↑ angular spread of the AOA φMS ↓ T̃ C (r) ↑.
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The Effect of κ on the BER Performance
4 5 6 7 8 9 1010
−4
10−3
10−2
10−1
100
Eb /N
0 (dB)
B i t e r r o r r a
t e
κ = 0
κ = 20
κ = 30
κ = 40
Coding system: 4-D 16QAM linear 32-state space-time trellis code with 2 transmit and 2 receiveantennas (δ BS = 30λ and δ MS = 3λ).
Observations: • κ ↑ angular spread ↓ BER ↑• If κ decreases from 40 to 0, then a gain of ca. 1.5 dB can be achieved at a BER
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VI. Conclusion
a The principle of deterministic channel modelling has been generalized.
a The generalized concept has been applied on the geometrical one-ring scattering model.
a It has been shown how the parameters of the simulation model can be determined by using the
L p-norm method (LPNM).
a The designed deterministic MIMO channel simulator with N = 25 scatterers has nearly the
same statistics as the underlying stochastic reference model with N = ∞ scatterers.
a The new MIMO space-time channel simulator is very useful in the investigation of the PDF,
LCR, and ADF of the channel capacity C (t) from time-domain simulations.
a Finally, it has been demonstrated that the system performance decreases if the spatial correlation
increases.
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