Paul AlexanderSKA Computational Challenges Square Kilometre Array Computational Challenges Paul Alexander.

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Paul AlexanderSKA Computational Challenges Square Kilometre Array Computational Challenges Paul Alexander

Paul AlexanderSKA Computational Challenges eVLA 27 27m dishes Longest baseline 30km GMRT 30 45m dishes Longest baseline 35 km E-MERLIN What is the Square Kilometre Array (SKA) Next Generation radio telescope – compared to best current instruments it is... ~100 times sensitivity ~ 10 6 times faster imaging the sky More than 5 square km of collecting area on sizes 3000km

Paul AlexanderSKA Computational Challenges What is the Square Kilometre Array (SKA) Next Generation radio telescope – compared to best current instruments it is... ~100 times sensitivity ~ 10 6 times faster imaging the sky More than 5 square km of collecting area on sizes 3000km Will address some of the key problems of astrophysics and cosmology (and physics) Builds on techniques developed in Cambridge It is an interferometer Uses innovative technologies... Major ICT project Need performance at low unit cost

Paul AlexanderSKA Computational Challenges Dishes

Paul AlexanderSKA Computational Challenges Phased Aperture array

Paul AlexanderSKA Computational Challenges also a Continental sized Radio Telescope Need a radio-quiet site Very low population density Large amount of space Possible sites (decision 2012) Western Australia Karoo Desert RSA

Paul AlexanderSKA Computational Challenges Sensitivity comparison SKA2 SKA1 LOFAR EVLA

Paul AlexanderSKA Computational Challenges ~ 250 Dense Aperture Array Stations MHz ~ 2700 Dishes Wide Band Single Pixel Feeds Phased Array Feeds 800 MHz – 2GHz ~250 Sparse Aperture Array Stations MHz 3-Core Central Region SKA2 Artist renditions from Swinburne Astronomy Productions

Paul AlexanderSKA Computational Challenges ~ 300 Dishes Wide Band Single Pixel Feeds ~50 Sparse Aperture Array Stations MHz 2-Core Central Region SKA1 Artist renditions from Swinburne Astronomy Productions

Paul AlexanderSKA Computational Challenges SKA Timeline 2019Operations SKA : Operations SKA Construction of Full SKA, SKA 2 €1.5B % SKA construction, SKA 1 €300M 2012Site selection Pre-Construction: 1 yr Detailed design€90M PEP 3 yr Production Readiness System design and refinement of specification Initial concepts stage Preliminary ideas and R&D

Paul AlexanderSKA Computational Challenges Work Packages in the PEP 1.Management 2.System 3.Science 4.Maintenance and support /Operations Plan 5.Site preparation 6.Dishes 7.Aperture arrays 8.Signal transport & networks 9.Signal processing 10.Science data processor 11.Telescope manager 12.Power SPO Work Package Contractors

Paul AlexanderSKA Computational Challenges UK (lead), AU (CSIRO…), NL (ASTRON…) South Africa SKA, Industry (Intel, IBM…) UK (lead), AU (CSIRO…), NL (ASTRON…) South Africa SKA, Industry (Intel, IBM…) Work Packages in the PEP 1.Management 2.System 3.Science 4.Maintenance and support /Operations Plan 5.Site preparation 6.Dishes 7.Aperture arrays 8.Signal transport & networks 9.Signal processing 10.Science data processor 11.Telescope manager 12.Power SPO Work Package Contractors

Paul AlexanderSKA Computational Challenges Very Brief Introduction to Radio Astronomy Imaging

Paul AlexanderSKA Computational Challenges XXXXXX SKY Image Detect & amplify Digitise & delay Correlate Process Calibrate, grid, FFT Integrate  visibilities s B B. s 12 Astronomical signal (EM wave) Visibility: V(B)= E 1 E 2 * = I(s) exp( i  B.s/c ) Resolution determined by maximum baseline  max ~ / B max Field of View (FoV) determined by the size of each dish  dish ~ / D Standard interferometer

Paul AlexanderSKA Computational Challenges Aperture arrays XXXXXX SKY Image Digitise, delay & beam form Correlate Process Calibrate, grid, FFT Beam form: Apply delay gradients to point electrically Multiple delay gradients  many beams and large FoV

Paul AlexanderSKA Computational Challenges Aperture arrays XXXXXX SKY Image Digitise, delay & beam form Correlate Process Calibrate, grid, FFT Beam form: Apply delay gradients to point electrically Multiple delay gradients  many beams and large FoV Aperture-Array station  ~25000 phased elements  Equivalent to one dish  These are then cross-correlated Aperture-Array station  ~25000 phased elements  Equivalent to one dish  These are then cross-correlated

Paul AlexanderSKA Computational Challenges Formulation What we measure from a pair of telescopes: In practice we have to deal with this equation, but for simplicity consider a scalar model s m l The delays allow us to follow a point on the sky The J i are direction dependent Jones matrices which include the effects of:  propagation from the sky through the atmosphere  scattering  coupling to the antenna/detector  gain The delays allow us to follow a point on the sky The J i are direction dependent Jones matrices which include the effects of:  propagation from the sky through the atmosphere  scattering  coupling to the antenna/detector  gain

Paul AlexanderSKA Computational Challenges Formulation Where we include time delays to follow a central point. In terms of direction cosines relative to the point we follow and for a b = (u,v,w) If we can calibrate our system we can apply our telescope-dependent calibrations and then for small FoV we can approximate And the measured data are just samples of this function In this case we can estimate the sky via Fourier inversion and deconvolution s m l

Paul AlexanderSKA Computational Challenges Formulation s m l Sampling of the Fourier plane is determined by the positioning of the antennas and improved by the rotation of the earth ee

Paul AlexanderSKA Computational Challenges The Science Aims and the Imaging Challenges

Paul AlexanderSKA Computational Challenges SKA Key Science Drivers ORIGINS  Neutral hydrogen in the universe from the Epoch of Re-ionisation to now When did the first stars and galaxies form? How did galaxies evolve? Role of Active Galactic Nuclei Dark Energy, Dark Matter  Cradle of Life FUNDAMENTAL FORCES  Pulsars, General Relativity & gravitational waves  Origin & evolution of cosmic magnetism TRANSIENTS (NEW PHENOMENA) Science with the Square Kilometre Array (2004, eds. C. Carilli & S. Rawlings, New Astron. Rev., 48)

Paul AlexanderSKA Computational Challenges Galaxy Evolution back to z~10? ~ 3000 galaxies~15 radio sources HDFVLA

Paul AlexanderSKA Computational Challenges HDFSKA Galaxy Evolution back to z~10?

Paul AlexanderSKA Computational Challenges The Imaging Challenge This illustrates one of our main challenges To make effective use of the improved sensitivity we face an immediate problem Typically within the field of view of the telescope the noise level will be ~10 6 – 10 7 times less than the peak brightness We have to achieve sufficiently good calibration and image fidelity to routinely achieve a “dyanamic range” of > 10 7 :1 With very hard work now we can just get to 10 6 :1 in some fields

Paul AlexanderSKA Computational Challenges The Processing Challenge

Paul AlexanderSKA Computational Challenges SKA 2 wide area data flow 16 Tb/s4 Pb/s 24 Tb/s 20 Gb/s

Paul AlexanderSKA Computational Challenges SKA1 Data rates from receptors Dishes –Depends on feeds, but illustrate by 2 GHz bandwidth at 8-bits –G = 64 Gb/s from each dish For Phased Array feeds increased by number of beams (~20) –G ~ 1 Tb/s For Low frequency Aperture Arrays : –Bandwidth is 380 MHz –Driven by the requirements of Field of View from the science requirements which from DRM is 5 sq-degrees  20 beams –G = 240 Gb/s These are from each collector into the correlator or beam former –300 dishes – m AA stations –G(total) ~ 68 Tb/s

Paul AlexanderSKA Computational Challenges Data Rates After correlation the data rate is fixed by straightforward considerations  Must sample fast enough (limit on integration time)  t  Baseline  B/  UV (Fourier) cell size  D/  Must have small-enough channel width to avoid chromatic aberration max  t max  – 

Paul AlexanderSKA Computational Challenges Data rates from the correlator Standard results for integration/dump time and channel width Data rate then given by # antennas # polarizations # beams word-length Can reduce this using baseline-dependent integration times and channel widths

Paul AlexanderSKA Computational Challenges Aperture Array Line experiment (e.g. EoR) 5 sq degrees; channels over 250 MHz bandwidth  ~ 30 GB/s reducing quickly to ~ 1GB/s  Up to 500 TB UV (Fourier) data; Images (3D) ~ 1.5 TB Continuum experiment with long baselines with the AA 100 km baseline with the low-frequency AA  1.2 TB/s reducing to ~ 12.5 GB/s  Up to 250 TB/day to archive if we archive raw UV data Spectral-line imaging with dishes  Data rates ~ 50 GB/s; Images (3D) ~ 27 TB Example correlator data rates and products SKA1

Paul AlexanderSKA Computational Challenges Pulsar search Galactic-plane survey for pulsars  ~ 400 GB/s to de-disperser (hardware?)  Data products are of small volume as all analysis is done in pseudo real-time. Example beam-formed data rates SKA1

Paul AlexanderSKA Computational Challenges Example Data rates SKA2

Paul AlexanderSKA Computational Challenges Data Products ~0.5 – 10 PB/day of image data Source count ~10 6 sources per square degree ~10 10 sources in the accessible SKA sky, 10 4 numbers/record ~1 PB for the catalogued data 100 Pbytes – 3 EBytes / year of fully processed data

Paul AlexanderSKA Computational Challenges Processing model

Paul AlexanderSKA Computational Challenges The SKA Processing Challenge CorrelatorVisibility processors switch AA: 250 x 16 Tb/s Dish: 3000 x 60 Gb/s Image formation Science analysis, user interface & archive ~ PFlop ~ ? PFlop Software complexity ~1 – 500 Tb/s ~ 200 Pflop to 2.5 Eflop

Paul AlexanderSKA Computational Challenges Conclusions The next generation radio telescopes offer the possibility of transformational science, but at a cost A major processing challenge Need to analyse very large amounts of streaming data Current algorithms iterative – need to buffer data Problem too large to, for example, use a direct Bayesian approach Are our (approximate) algorithms good enough to take into account all error effects that need to be modelled? Only recently have we had to consider most of the effects – what have we forgotten? Phased approach to SKA is very good for the processing – performance increasing and critically we can continually learn

Paul AlexanderSKA Computational Challenges