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Main beam representation in non-regular arrays

Main beam representation in non-regular arrays. Christophe Craeye 1 , David Gonzalez-Ovejero 1 , Eloy de Lera Acedo 2 , Nima Razavi Ghods 2 , Paul Alexander 2. 1 Université catholique de Louvain, ICTEAM Institute 2 University of Cambridge, Cavendish Laboratory.

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Main beam representation in non-regular arrays

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  1. Main beam representation in non-regular arrays Christophe Craeye1, David Gonzalez-Ovejero1, Eloy de Lera Acedo2, NimaRazavi 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

  2. 2 parts Preliminary: Patterns of apertures – a review Next: analysis of aperture arrays with mutual coupling Algarve meeting, 2011

  3. a b r Algarve meeting, 2011

  4. Fourier-Bessel series Algarve meeting, 2011

  5. Zernike series NB: the Zernike function is a special case of the Jacobi Function Algarve meeting, 2011

  6. Zernike functions Picture from Wikipedia CALIM 2011

  7. Radiation pattern Hankel transform Algarve meeting, 2011

  8. F.T. of Bessel Algarve meeting, 2011

  9. FT of Zernike Algarve meeting, 2011

  10. Sparse polynomial Algarve meeting, 2011

  11. Context: SKA AA-lo Non-regular: max effective area with min nb. elts w/o grating lobes. CALIM 2011

  12. 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

  13. 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

  14. Outline Limits of traditional coupling correction Array factorization Array factors: series representations Reduction through projection Scanning Algarve meeting, 2011

  15. 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 CALIM 2011

  16. 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. CALIM 2011

  17. Mutual coupling correction Half-wave dipole Isolated Embedded Corrected CALIM 2011

  18. Mutual coupling correction Bowtie antenna l=1.2 m, l=3.5 m Isolated Embedded Corrected CALIM 2011

  19. 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 ~ CALIM 2011

  20. Multiple-mode approach Macro Basis Functions(Suter & Mosig, MOTL, 2000, cf. also Vecchi, Mittra, Maaskant,…) a + b + g + d MBF 2 MBF 4 MBF 1 MBF 3 CALIM 2011

  21. C111 C211 C311 MBF 1 C122 C222 C322 MBF 2 Array factorisation Z L s n Antenna index Coefficients for IDENTICAL current distribution … CALIM 2011

  22. C111 C211 C311 MBF 1 C122 C222 C322 MBF 2 Array factorisation Z L s n Antenna index Coefficients for IDENTICAL current distribution … CALIM 2011

  23. Example array - Array radius = 30λ0. - Number of elements = 1000. λ0 - Distance to ground plane = λ0/4. - No dielectric. λ0 Z = 200Ω CALIM 2011

  24. Random arrangement Random configuration ~ 35 dB E-plane H-plane CALIM 2011

  25. Quasi-random arrangement CALIM 2011

  26. Radius of Influence 100 elements 1000 elements 10 elements H-plane ICEAA 2011

  27. Aperture sampling (1) CALIM 2011

  28. Aperture sampling (2) Define a local density (several definitions possible) CALIM 2011

  29. Aperture scanning (1) CALIM 2011

  30. Aperture scanning (2) CALIM 2011

  31. Patterns versus size of array CALIM 2011

  32. Coherent & incoherent regimes ~ ~ 0.3 Number of sidelobes in “coherent” regime CALIM 2011

  33. Aperture field representation a b CALIM 2011

  34. Pattern representation Angle from broadside CALIM 2011

  35. Polynomial decomposition CALIM 2011

  36. Fourier-Bessel decomposition = CALIM 2011

  37. 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. 2539-2551, Aug. 2010. CALIM 2011

  38. 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. 425-435, Jul. 1980. CALIM 2011

  39. CALIM 2011

  40. Array factor with apodization CALIM 2011

  41. Array factor with apodization CALIM 2011

  42. Apodization function w(r) extracted CALIM 2011

  43. Approximate array factor extracted 20 % error on amplitudes l/4 error on positions (at 300 MHz) CALIM 2011

  44. Residual error with Z-B approach CALIM 2011

  45. Residual error with Z-B approach CALIM 2011

  46. Residual error with Z-B approach CALIM 2011

  47. Residual error with Z-B approach CALIM 2011

  48. Residual error with Z-B approach CALIM 2011

  49. Residual error with Z-B approach CALIM 2011

  50. Residual error with Z-B approach CALIM 2011

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