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Published byAmelia Lawrence Modified over 9 years ago
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Main beam representation in non-regular arrays
Christophe Craeye1, David Gonzalez-Ovejero1, Eloy de Lera Acedo2, Nima Razavi Ghods2, Paul Alexander2 1Université catholique de Louvain, ICTEAM Institute 2University of Cambridge, Cavendish Laboratory CALIM 2011 Workshop, Manchester, July 25-29, 2011 2d calibration Workshop, Algarve, Sep 26, 2011
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2 parts Preliminary: Patterns of apertures – a review
Next: analysis of aperture arrays with mutual coupling Algarve meeting, 2011
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a b r Algarve meeting, 2011
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Fourier-Bessel series
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Zernike series Algarve meeting, 2011
NB: the Zernike function is a special case of the Jacobi Function Algarve meeting, 2011
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CALIM 2011 Zernike functions Picture from Wikipedia
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Radiation pattern Hankel transform Algarve meeting, 2011
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F.T. of Bessel Algarve meeting, 2011
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FT of Zernike Algarve meeting, 2011
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Sparse polynomial Algarve meeting, 2011
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Context: SKA AA-lo CALIM 2011
Type of element Bowtie Spiral Log-periodic Non-regular: max effective area with min nb. elts w/o grating lobes. Parameter Specification Low frequency 70 MHz High frequency 450 MHz Nyquist sampling frequency 100 MHz Number of stations 50 => 250 Antennas per station 10.000 CALIM 2011
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Problem statement Goal: pattern representation for all modes of operation at station level. Too many antennas vs. number of calibration sources Calibrate the main beam and first few sidelobes Suppress far unwanted sources using interferometric methods (open). Compact representations of patterns, inspired from radiation from apertures, including effects of mutual coupling Algarve meeting, 2011
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Specific to SKA AAlo Fairly circular stations (hexagonal would be OK)
Relatively dense Weak amplitude tapering – some space tapering Irregular => all EEP’s very different Even positions are not 100 % reliable (within a few cm) Correlation matrix not available Nb. of beam coefficients << nb. Antennas Restrict to main beam and first few sidelobes Even assuming identical EEP’s and find 1 amplitude coefficient per antenna is way too many coefficients Algarve meeting, 2011
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Outline Limits of traditional coupling correction Array factorization
Array factors: series representations Reduction through projection Scanning Algarve meeting, 2011
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Embedded element pattern
CALIM 2011 Embedded element pattern Z L Impedance isolated elt Array impedance matrix To get voltages in uncoupled case: multiply voltage vector to the left by matrix
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Embedded element pattern
CALIM 2011 Embedded element pattern Z L After correction, we are back to original problem, with (zoomable, shiftable) array factor Gupta, I., and A. Ksienski (1983), Effect of mutual coupling on the performance of adaptive arrays, IEEE Trans. Antennas Propag., 31(5), 785–791.
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Isolated Embedded Corrected
CALIM 2011 Mutual coupling correction Half-wave dipole Isolated Embedded Corrected
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Isolated Embedded Corrected
CALIM 2011 Mutual coupling correction Bowtie antenna l=1.2 m, l=3.5 m Isolated Embedded Corrected
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Mutual coupling correction
CALIM 2011 Mutual coupling correction Bowtie antenna l=1.2 m, l=1.5 m Isolated Embedded Corrected SINGLE MODE assumption not valid for l < l/2 ~
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Multiple-mode approach
CALIM 2011 Multiple-mode approach Macro Basis Functions (Suter & Mosig, MOTL, 2000, cf. also Vecchi, Mittra, Maaskant,…) a b g d MBF 1 MBF 2 MBF 3 MBF 4
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Array factorisation … CALIM 2011 Z L s n Antenna index C111 C211 C311
MBF 1 MBF 2 Coefficients for IDENTICAL current distribution …
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Array factorisation … CALIM 2011 Z L s n Antenna index C111 C211 C311
MBF 1 MBF 2 Coefficients for IDENTICAL current distribution …
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Example array CALIM 2011 - Array radius = 30λ0.
- Number of elements = 1000. λ0 - Distance to ground plane = λ0/4. - No dielectric. λ0 Z = 200Ω
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Random arrangement CALIM 2011 Random configuration ~ 35 dB E-plane
H-plane
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Quasi-random arrangement
CALIM 2011 Quasi-random arrangement
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Radius of Influence H-plane ICEAA 2011 1000 elements 100 elements
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CALIM 2011 Aperture sampling (1)
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(several definitions possible)
CALIM 2011 Aperture sampling (2) Define a local density (several definitions possible)
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CALIM 2011 Aperture scanning (1)
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CALIM 2011 Aperture scanning (2)
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Patterns versus size of array
CALIM 2011 Patterns versus size of array
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Coherent & incoherent regimes
CALIM 2011 Coherent & incoherent regimes ~ ~ 0.3 Number of sidelobes in “coherent” regime
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Aperture field representation
CALIM 2011 Aperture field representation b a
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Pattern representation
CALIM 2011 Pattern representation Angle from broadside
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Polynomial decomposition
CALIM 2011 Polynomial decomposition
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Fourier-Bessel decomposition
CALIM 2011 Fourier-Bessel decomposition =
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Fourier-Bessel decomposition
CALIM 2011 Fourier-Bessel decomposition = A. Aghasi, H. Amindavar, E.L. Miller and J. Rashed-Mohassel, “Flat-top footprint pattern synthesis through the design of arbitrarily planar-shaped apertures,” IEEE Trans. Antennas Propagat., Vol. 58, no.8, pp , Aug
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Zernike-Bessel decomposition
CALIM 2011 Zernike-Bessel decomposition Y. Rahmat-Samii and V. Galindo-Israel, “Shaped reflector antenna analysis using the Jacobi-Bessel series,” IEEE Trans. Antennas Propagat., Vol. 28, no.4, pp , Jul
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CALIM 2011 Polynomial Fourier-Bessel Zernike-Bessel Fast functions Good 1st order weaker at low orders weak direct convergence fast direct convergence
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CALIM 2011 Array factor with apodization
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CALIM 2011 Array factor with apodization
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Apodization function w(r) extracted
CALIM 2011 Apodization function w(r) extracted
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Approximate array factor extracted
CALIM 2011 Approximate array factor extracted 20 % error on amplitudes l/4 error on positions (at 300 MHz)
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach
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CALIM 2011 Density function The number of terms tells the “resolution” with which density is observed
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Array of wideband dipoles
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AF convergence Over just main beam
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AF convergence Main beam + 1st sidelobe
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Project on 1, 2, 3 MBF patterns at most
AF convergence Project on 1, 2, 3 MBF patterns at most Algarve meeting, 2011
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Pattern projections Power radiated by MBF pattern 0
NB: can be projected on more than 1 (orthogonal) MBFs
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Full pattern Algarve meeting, 2011
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Error w/o MC Algarve meeting, 2011
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Error after pattern projection
Only 1 pattern used here (pattern of “primary”) Algarve meeting, 2011
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l =0.0 Algarve meeting, 2011
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l =0.1 Algarve meeting, 2011
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l =0.2 Algarve meeting, 2011
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l =0.3 Algarve meeting, 2011
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l =0.4 Algarve meeting, 2011
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l =0.5 Algarve meeting, 2011
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l =0.6 Algarve meeting, 2011
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Variation of maximum Real Imaginary Algarve meeting, 2011
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Conclusion Representation based on array factorization
Projection of patterns of MBF on 1 or 2 of them Representation of array factors with functions use for apertures (done here with 1 array factor) Array factor slowly varying when shifted upon scanning (to be confirmed with more elements and other elt types) Algarve meeting, 2011
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