AA_PhD_MIMO_802_11n
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Transcript of AA_PhD_MIMO_802_11n
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Channel models for MIMO
Adaptive Antenna Systems
Persa Kyritsi
December 16, 2004
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What you are going to learn today:
Fundamentals of MIMO systems Transmission techniques for MIMO
Channel models for MIMO
(details on 802.11n)
Real MIMO measurements
Power
Capacity Rate
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Why do we need channel models?
Prediction models for site planning Site specificAntenna dependent
Accurate Models for system design and algorithm
testing
Site and antenna independent
Tolerance for lower accuracy
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Classification of MIMO channel models
MIMO channel models
Deterministic Stochastic
Recordedimpulse
responses
Ray-tracingtechnique
Geometricallybased
Parametricstochastic
Correlationbased
Non-physical
Physical
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Correlation based models
kiljhh RXTXklij ,,, Kronecker assumption:
Separability of transmit and receive correlations
NN
MM
vec
RX
TX
iidRXTXvec
TT
M
TT
vec
M
:
:
HH
HHHH
HHH
21
21
21
R
R
RR
H
H
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How to calculate the correlations
PAS(
): Power Azimuth Spectrum(how much energy is arriving from where)
How do the correlations look?
dPASdkdR
dPASdkdR
djRdRd
lXYl
lXXl
XYlXXlIQl
sin
,cos
,
,
,,
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Discussion
Simple & elegant Experimental validation in some environments and
discrediting in others
Original expression cannot capture the pinhole
effect
Generalization:
212121
TXtsrRX RHRHRH
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MIMO channels: Wideband
Narrowband Wideband
l
l
l
l
ttt
tnttxtyMIMO
tthth
tnttxhtySISO
HH
H:
:
1
0
1
0
:
:
L
l
ll
L
lll
ttt
tntxttyMIMO
tthth
tntxthtySISO
HH
H
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A specific example: 802.11n
Develop a MIMO channel model for 802.11channels
Applicable to
Environments where 802.11 systems are to beused Both 2.4GHz and 5GHz bands
Approach
From narrowband to broadband From SISO to MIMO
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MIMO channels: Narrowband
TRANSMITTERS RECEIVERS
1
2
M
1
2
N
y = Hx + n
xj: transmitted signal from tx j
yi: received signal on rx i
ni
: noise on rx i
hij: From tx j to rx i (hijC)
h11
h12
h1M
h21
h22
h2M
hN1
hN2
hNM
IR2nn
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802.11n Channel model
SISO channel models (Medbo 98):Tap delay line model for various envts
MIMO channel models (Erceg et al 03):
Correlation-based model
Clustering in
Time (Saleh-Valenzuela)Angle (AoA and AoD)
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Additional parameters in 802.11n MIMO
channel models
Local signal statistics (Ricean/ Rayleigh)
Polarization Doppler spectrum
Power roll-off law
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Interdependence of parameters
ds AS The distribution is always Laplacian Value selected to match experimental results
d More Rayleigh than Ricean
(LOS for d< dBP, NLOS for d>dBP)
ds K
Value selected to match experimental results
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SISO Channel Models
Model Environment LOS Delay spread
A Office No 50ns
B
Large open
space/ Office No 100ns
CLarge open
spaceNo 150ns
D
Large open
space YES 140ns
ELarge open
spaceNo 250ns
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MIMO Channel Models
Model Environment Scatteringsituation Delay spread
A Narrowband LOS/NLOS 0ns
B ResidentialLOS(K=0)/
NLOS15ns
C Residential/ Small officeLOS(K=0)/
NLOS30ns
D (A) OfficeLOS(K=3)/
NLOS50ns
E (B) Large open space/ OfficeLOS(K=6)/
NLOS100ns
F (C) Large open spaceLOS(K=6)/
NLOS150ns
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From SISO to MIMO
SISO channel
MIMO channel
0
1,l
0
3,l
0
2,l
1,l
2,l
3,l
(Clustering in time)
(Clustering in time & angle)
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From SISO to MIMO
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From SISO to MIMO
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From SISO to MIMO
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From SISO to MIMO
1,l
0
1,l
0
2,l
2,l
Tap 4
0
1,l
0
2,l
1,l
2,l
Tap 5
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Additional parameters (I)
Local signal statistics(LOS for d< dBP, NLOS for d>dBP)
Polarization
LOS: 3dB X-pol discrimination
NLOS: 10dB X-pol discrimination
dBP
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Additional parameters (II)
Doppler spectrum Bell shaped
Possibly: Spike due to moving vehicle Effect of fluorescent ligths
2
1
1)(
df
fA
fS
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Additional parameters (III)
Power roll-off law Exponential power roll-off
Log normal distribution Log normal variance depends on
The distance from the TX The environment
BP
BP
BPFS
BPFS
ddd
ddL
dddL
dL ,log5.3
,
10
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Simulation methodology
Define parameters M, N Type of environment
Distance from source For each tap
Calculate RTx and RRX Generate independent samples & filter through R
Tx
and RRX
Add LOS component if there is such Filter through Doppler filter
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Limitations of the model
The model can be usedfor any array geometry
Simulation software
free
Angular parameters arehard-wired (both for
LOS and scattered
components)
Change from LOS toNLOS is more gradual
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The reality