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John Kot, CSIRO

A Luneburg Lens for the SKA Summary of the MNRF research project into the manufacture of a low-cost microwave refracting spherical lens for radioastronomy. John Kot, CSIRO. Ren é Magritte: “Voice of Space”. The vision: a spherical lens seeing the whole radio sky.

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John Kot, CSIRO

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  1. A Luneburg Lens for the SKASummary of the MNRF research project into the manufacture of a low-cost microwave refracting spherical lens for radioastronomy John Kot, CSIRO René Magritte: “Voice of Space”

  2. The vision: a spherical lens seeing the whole radio sky • The full bandwidth and collecting area of the telescope is available for multiple, simultaneous, independent users.

  3. The classical Luneburg lens is a spherically-symmetric, graded index lens which images a point on the celestial sphere to a point on the lens surface. A practical lens would comprise uniform shells, with focus away from the lens surface. Spherical microwave lenses

  4. Materials development

  5. Dielectric lens materials • Simple calculation based on the dielectric properties of polymer foam and the price of raw materials (oil) shows that a foamed polymer lens would be far too expensive for the SKA • Only artificial materials seem to offer low loss and low density.

  6. Artificial dielectrics • Artificial dielectrics are made by distributing small polarizable particles in a uniform background material – a macroscopic analogue of a “natural” dielectric. • Controllable dielectric properties • Reduced loss and density • Two main classes: • Metallic particles (traditional artificial dielectric) • Dielectric particles (composite dielectrics)

  7. Nike-Zeus acquisition radar 90 ft

  8. Measured results for Cu wire artificial crystal Structure 2 Structure 1

  9. Composite dielectrics • Candidate material is a composite of ceramic particles in low-density polymer foam. • Ceramics: Titanium dioxide has high dielectric constant (100), is widely used in microwave components, and is available cheaply in large quantities (paint pigment) • Standard industrial processes can mass-produce loaded polymer foams.

  10. The dielectric properties of a dielectric mixture depend strongly on the distribution of the different fractions of the composite. Two mixtures of identical amounts of the same materials can have radically different properties. Physics of dielectric mixtures Inverse opal Opal

  11. Dielectric constant for different TiO2 mixtures: opal & inverse opal 100 inverse opal dielectric constant opal 80 60 40 20 0 0 0.2 0.4 0.6 0.8 1 volume fraction

  12. Random mixture of Al2O3 disks in EPS

  13. Development of a shaped ceramic particle composite • Shaped particles can approach an ideal mixture. • Production method for shaped TiO2 particles developed by CSIRO MIT, including extensive work on doping to reduce loss • Polymer foam extrusion process compatible with TiO2 particles developed by CSIRO MS • Production of simple shapes by moulding process • Material design and measurement done by CSIRO TIP / ICT Centre

  14. Effective dielectric constant for uniform random mixture of TiO2 disks in air 2.2 dielectric constant 2 1.8 1.6 1.4 1.2 1 2% 1% 0 fractional volume of inclusions

  15. Measured results for TiO2 plates in EPS

  16. Limitation of the current material 100 Eccentricity: 1:1 10:1 30:1 100:1 80 60 dielectric constant 40 20 0 0 0.5 1 volume fraction The ideal mixing rule is approached by high eccentricity particles. The present extrusion process limits the eccentricity to around 30:1, giving roughly 6x increase in density.

  17. Manufacturing a prototype lens

  18. Manufacture & testing of a 1m prototype lens Trial assembly of lens parts The lens arrives at Marsfield

  19. Manufacture & testing of a 1m prototype lens Testing in the antenna range Radiometric measurement of material loss

  20. Results for prototype lens • Dielectric loss: excellent; loss tangent < 10-4 • Uniformity: good; OK for < 10 GHz; some further development needed for >10 GHz • Manufacturing by moulding process: successful proof of concept • Density: Approximately 20% improvement over foamed polymer lens, but still 6x higher than theoretical limit, due to limitations of extrusion process • Isotropy: Poor; limits efficiency above 4 GHz; caused by excessive compression during moulding

  21. Conclusions • The project has studied the feasibility of refracting spherical lenses for the SKA, and found that both metal wire artificial crystals and TiO2-based composite dielectrics could in principle be used to manufacture lenses at low cost and low loss. • A TiO2-based composite dielectric material has been developed, and a proof-of-concept prototype lens successfully produced with a process scalable to cheap mass production. The IP is protected by a provisional patent.

  22. Conclusions (II) • The performance of the current material is limited by the manufacturing process we have available. Within the budget & time limits of the NTD project there is no realistic prospect of developing the new manufacturing process needed to advance the lens development. • Under the current project, we plan to round off the current work to the stage where it can be easily picked-up again in the future, should the need or will arise.

  23. Conclusions (III) • CSIRO will extend the current patent for 3 years, and actively seek partners for commercial and scientific application of the technology such as: • CSIRO’s wideband dielectric-loaded feed horn technology, as used by project SETI • Use of small spherical lenses for Ka-band mobile satcom applications, e.g. video surveillance by UAVs. • The hybrid lens / aperture array proposal presented by Peter Hall at Capetown remains the most attractive option for the SKA that offers unconstrained multiple fields-of-view across the SKA frequency band

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