alain sibille (sibille@ensta.fr), stéphane fassetta*sibille@ensta.fr laboratoire...

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Alain SIBILLE (sibille@ensta.fr), Stéphane FASSETTA*

Laboratoire Electronique-InformatiqueENSTA, 32 Bd Victor, 75739 Paris cedex 15, France

* Now at THALES Communications, Colombes, France

INTERSECTOR CORRELATIONS FOR SWITCHED BEAMS DIVERSITY PERFORMANCE EVALUATION

Outline

context and motivation

antennas

intersector correlations: theory

computations assuming a model scenario

comparison with experimental results

angular vs. spatial diversity

conclusion

Context and motivation

GENERAL CONTEXT: low-complexity beam-switched smart antennas for

terminals, HIPERLAN 2 access points etc …

MOTIVATION: an attempt to quantify the potential benefit brought by beam-

switched antennas prior to any experiment, intended for optimal antenna design.

PARTICULAR CONTEXT: experimental channel measurement campaigns and

antenna design carried out within the European ADAMO project (1998-2000).

Antennas

  

6 monopoles circular array 4 patches planar array

  

6 BSSA circular array 13 monopoles array

Antennas

Intersector correlations : theory

)().(/)( ,,, HjHjHiHiHjHiij IEIEIE

dHHI jiHjHi )()( *

,

Hi

Hj

Wideband intersector correlation:

with

i

j

rij is a measure of the diversity performance of a switched beams antenna for wideband radio link (single or multiple carriers)

lllil

llilli

jkDBGF

dkDjgBFH

)exp()()()(

)()exp()()(2

1)(

ml

mlmjlimlHjHi kDkDBBEIE,

**, )()(2)(

l

llili gAfh )(.)()( Discrete multipath channel model:

f(t): receiver filter CIR Ail: path transmittance(Di: receiver antenna radiation pattern)

tl: path delay gl: CIR of environment+ emitter

)( lil kDB

2)()( GF)( : Fourier transform of

Intersector correlations : theory

dDDpIE jiHjHi ).,(),(.),(02)( *,

Di,j: radiation patternsP(): angular power spectrum for omni receiver antenna

Assuming perfect averaging of small-scale fading:

)()(02)( *2

, ljlill

HjHi kDkDBEIE

Continuous approximation of the discrete sum (scenario averaging):

Intersector correlation:

dDpdDp

dDDp

ji

ji

ij

.),(.),(.),(.),(

).,(),(.),(22

*

Intersector correlations : theory

The channel correlation contains the term:

Intersector correlations : theory

)()()()()()( ******ljlljllillilljllil kDBkDBkDBkDBEkDBkDBE

Extension to polarisation-dependent propagation

).,(

).,(),(

p

pXPD

)( ,HjHiIE

)()()()(

)()()()(

****

*2*2

ljlillljlill

ljlilljlil

kDkDBBkDkDBB

kDkDBkDkDBE

dDDp

dDDp

dDDp

ji

ji

ji

).,(),(.),(

).,(),(.),(

).,(),(.),(

*

*

*

),(),,(),,( ppp ),( pgeneralize

),( p is somewhat related to

Continuous approximation:

Computations assuming a V-V model scenario

/2exp2

1)(),( cpp

c

6 BSSA array

0 50 100 150 0

0.2

0.4

0.6

0.8

1

ANGLE (°)

CO

RR

EL

AT

ION

0°/10° 0°/40° 40°/10° 40°/40°

4 patches array

c

Complex vs. Amplitude-only correlations(Phase behavior)

0 50 100 150 0

0.2

0.4

0.6

0.8

1

ANGLE (°)

CO

RR

EL

AT

ION

0°/10° compl 40°/10° compl 0°/10° real

40°/10° real

13 monopoles array

Computations assuming a V-V model scenario

Comparison with experimental results(ADAMO campaign 1, IMST indoor measurements)

x

y

zplotter

table

table

table

locker

table

table

bookshelf

bookshelf

bookshelf

bookshelf

maga

zine rack

1.5 m

2 m

3.5 m

4.5 m

2.5m

a b c

d

zz z

y

x

y

y

x

x

y

z

x

blackbo

ard

Tx

5.25

3 rooms: small , library, hall 6 beams antenna at ceiling levelomnidirectional radiator at desk level5.2 GHz, 120° MHz BW31 locations, small-scale fading averaging every /106 monopoles array and 4 patches array

library

small office

  c (°) (°) =60° 

=120° 

=180° 

  0 5 0.46 0.13 0.15  0 10 0.46 0.12 0.16  0 20 0.48 0.10 0.16

 model:

0 40 0.50 0.07 0.15

20 10 0.56 0.03 0.07  20 20 0.56 0.03 0.07  20 40 0.55 0.02 0.08  30 20 0.60 0.09 0.01  30 40 0.58 0.06 0.04

CAMPAIGN 1 (6 monopoles array) 0.23 0.009 0.05

small office 0.31 0.07 0.07

library 0.25 0.11 0.04

hall 0.46 0.07 0.09

Comparison with experimental results

(ADAMO campaign 1, IMST measurements)

ADDITIONAL SPATIAL DIVERSITY

d

0 50 100 150 0

0.2

0.4

0.6

0.8

1

ANGLE (°)

CO

RR

EL

AT

ION

+0.2 +0.1 0 -0.1 -0.2

6 monopoles array d /

Computations assuming a V-V model scenario

INTERSECTOR CORRELATION: model vs. Experiment(ADAMO campaign 1)

 

c  60° 120° 180° d/

6Monop exp

0.290 0.069 0.030      

6Monop model

0.292 0.071 0.030 40 40 0.18

4Patches exp

0.144 0.037 0.019      

4Patches model

0.140 0.027 0.024 35 15 0.38

Comparison with experimental results

expected on account of the Tx-Rx LOS tilt in elevation

Angular vs. spatial diversity

spatial diversity = spatial filtering of faded signals

angular diversity = angular filtering of incoming waves

IS THERE A FUNDAMENTAL DIFFERENCE BETWEEN BOTH ? IS THE

DISTINCTION BETWEEN ANGULAR AND SPATIAL DIVERSITY SO

CLEAR IN PRACTICAL ARRAYS ?

ROLE OF THE PHASE CENTER

Angular vs. spatial diversity

y’

x’

z’

O

P

r

rk

N

M

k

(r, , )

z

y

x

(r, , )

6 points in angular space, used to locally equate to zero the phase differential

r

jkrjA

r

jkrErE O )),(exp(

),()exp(

),(),,( 00

« local » phase center for a given () direction

ROLE OF THE PHASE CENTER

A SIMPLE INTERPRETATION: sectored arrays also exhibit spatial diversity due to sector dependent position of the phase center

phase center

driven monopoles

reactively loaded monopoles

6 MONOPOLES ARRAY

Angular vs. spatial diversity

13 MONOPOLES ARRAY

y ( m m ) phase center

driven monopoles

reactively loaded monopoles 1

reactively loaded monopoles 2

short-circuited monopole

ROLE OF THE PHASE CENTER

Angular vs. spatial diversity

Conclusion

A simple tool has been proposed to evaluate the diversity performance of beam-

switched antennas: intersector correlations assuming a model scenario

Comparison with indoor propagation channel measurements is favorable, on

condition of the presence of extra spatial diversity

Evidence of hybrid spatial angular diversity in beam-switched circular arrays

due to non central position of the phase center.

Perspective: evaluation of correlations for MIMO antennas

Acknowledgements

The authors are grateful to J. Kunisch, M. Schneider, J. Pamp, E. Zollinger, A. Winkelman and M. Gehrt of IMST for supplying CIR measurements

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