Correlator design(s) Trade-offs 20 July 2009 Christian Holler/Kris Zarb Adami Oxford University.
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Transcript of Correlator design(s) Trade-offs 20 July 2009 Christian Holler/Kris Zarb Adami Oxford University.
Bolometer vs. Interferometer
Only about 25 bolometer beams (blue dots) fit over the cluster area, with a low filling factor due to thediffraction-limited single-mode optics. None of the other bolometers in the array (of which there may be athousand) contribute to the image. In contrast all the interferometer antennas point directly at the cluster.Background image is an actual interferometric image of a rich cluster at 30 GHz, made with a telescope(CBI2) with filling factor f = 0.7, Tsys = 35 K
Taking as a goal the requirement to correlate Nant = 90 antennas withB = 40GHz bandwidth and Nch = 8 frequency channels, the approximate number of operations required is:
Nop = 16B ln 2(Nch)Nant + 2Nant(Nant − 1)B = 815Top/s
assuming an FX correlator and a single polarization (four times larger for full polarization).
Digital FPGA/ASIC Correlators and Spectrometers
Multiplier replaced by digital logic, fourier transform replaced by complex multipliers
Largest advantage in F-X correlators specifically for spectroscopic science
Can be built quickly with Off-the-Shelf Products using standard FPGA(s) and network switches
Very stable, analogue and systematic effects (such as band-pass, differential mismatch) can be corrected
RFI Excision and other effects can be easily incorporated – an example of this could be a digital back-end to C-BASS which is possible with today’s technology
Easily programmable, possible use for on-the-fly systematic reduction, template matching
Digital Correlator Design Limitations
ADC front-end (max. of 8-bit 56 GSa/s reported in literature)
Network switch, Back-plane and inter-chip communications for large-N correlators
Processing capability and power consumption (~1 Top/s; ~300W)
Not likely in the next 5 years
BUT, digital spectrometers are possible
Wilkinson power dividerWPD2 0.1-30GHz
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