Processing & Properties of Floor and Wall Tiles.pptx
3D Spatial Channel Modeling
1. Spatial Channel Modeling Based on
Wave-field Representation
Pavel Loskot
University of Alberta, Edmonton, Alberta, Canada
June 14, 2002
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Presented in Finnish Wireless Communications Workshop, 2001, Tampere, Finland
2. Outline
How to apply electromagnetic (EM) theory to channel modeling in
communication signal processing ? i.e., signal wave
Overview of existing spatial channel models (literature)
A new approach to spatial channel modeling is suggested
A necessary EM theory background is discussed
The method illustrated on linear stochastic and geometrical channel
models
3. Why Spatial Channel Models ?
Conventional channel models (COST#207)
field-strength and signal delays only (tap-delay line)
omnidirectional Tx,Rx antennas
For multiple antennas (COST#259)
we may gain (some) access to spatial domain
need for more accurate (directional) channel model
(but backward compatibility with COST#207)
also useful to network planing and deployment
(macrocells, microcells, picocells in some frequency band)
7. Representation of Wireless Transmission
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let us assume a global 3D-space, time and frequency coordinates
could be an electromagnetic wave
signal,wave system (channel)
when does or form a channel impulse response ?
9. Antenna Representation
Electromagnetic wave
a function of time and space
, i.e., a time-varying field
fields are invariant w.r.t. coordinate system
scalar or vector fields; given ( ) we know ( )
Transmit Antenna
radiating (source) field
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where
ž
is carrier field (hence, amplitude modulator)
Receive Antenna
observable field
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where
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is time-invariant infinite bandwidth antenna response
11. Maxwell Theory
every medium: permitivity
²
, permeability
²
conductivity ; e.g.,
raindrops, trees, walls (dielectric material), cars (conductive material)
Homogeneous medium
propagation along straight lines (at least locally)
Dispersive medium
Isotropic
energy flow along the direction of propagation ( , direction
independent)
Linear
, and are independent of applied field
Maxwell equations are linear and superpozition applies
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16. Combined Geometrical and Stochastic Model
[Molisch, VTC’02, ICC’02]
generic model to study wave propagation in MIMO systems
independent of antenna configuration (polarization)
random scatterers with given distribution
local scatterers around Tx, Rx antennas
far scatterers, clusterring
waveguiding and diffraction (keyhole effect)
Channel reciprocity (uplink/downlink)
direction of arrival and departure (DOA, DOD)
2D model: azimuth, 3D model: azimuth and elevation
delays, mean powers
plus comlex path gains in time-duplex systems
18. References
[1] J. J. Blanz and P. Jung, “A flexibly configurable spatial model for
mobile radio channels,” IEEE Trans. Commun., vol. 46, no. 3, pp.
367–371, Mar. 1998.
[2] R. B. Ertel, P. Cardieri, K. W. Sowebry, T. S. Rappaport, and J. H.
Reed, “Overview of spatial channel models for antenna array
communication systems,” IEEE Per. Comm., vol. 5, no. 1, pp. 10–22,
Feb. 1998.
[3] B. H. Fleury, “First- and second-order characterization of direction
dispersion and space selectivity in the radio channel,” IEEE Trans.
Inform. Th., vol. 46, no. 6, pp. 2027–2044, Sept. 2000.
[4] T. Zwick, C. Fischer, D. Didascalou, and W. Wiesbeck, “A stochastic
spatial channel model based on wave-propagation modeling,” IEEE
J. Select. Areas Commun., vol. 18, no. 1, pp. 6–15, Jan. 2000.
19. References
[5] Z. Ji, B.-H. Li, H.-X. Wang, H.-Y. Chen, and T. K. Sarkar, “Efficient
ray-tracing methods for propagation prediction for indoor wireless
communications,” IEEE Ant. Prop., vol. 43, no. 2, pp. 41–49, Apr.
2001.
[6] A. F. Molisch, J. Laurila, K. Hugl, and E. Bonek, “Smart antennas
and mimo systems,” in Proc. VTC, 2002, Tutorial.
[7] A. F. Molisch, “A generic model for mimo wireless propagation
channels,” in Proc. ICC, 2002, vol. 1, pp. 277–282.
[8] M. Steinbauer, A. F. Molisch, and E. Bonek, “The double-directional
radio channel,” IEEE Ant. Prop., vol. 43, no. 4, pp. 51–63, Aug.
2001.