MeerKAT Large Survey Projects SAAO Board, Roy Booth (SA SKA Project)

Slides:



Advertisements
Similar presentations
CNR ISTITUTO DI RADIOASTRONOMIA INAF Sardinia Radio Telescope G. Grueff IRA – Istituto di Radioastronomia INAF – Istituto Nazionale di Astrofisica.
Advertisements

Observations of the evolution of HI in galaxies across different environments. D.J. Pisano (West Virginia University)
The W i d e s p r e a d Influence of Supermassive Black Holes Christopher Onken Herzberg Institute of Astrophysics Christopher Onken Herzberg Institute.
HI Stacking: Past, Present and Future HI Pathfinder Workshop Perth, February 2-4, 2011 Philip Lah.
Deep Neutral Hydrogen Surveys with the Arecibo 305-m Telescope – the Arecibo Galaxy Environment Survey Robert Minchin NAIC Arecibo Observatory.
The Cosmic Evolution of Neutral Atomic Hydrogen Gas University of Sydney Colloquium 27 November 2014 Philip Lah.
Mapping HI absorption at z=0.026 against a resolved background CSO Andy Biggs, Martin Zwaan, Jochen Liske European Southern Observatory Frank Briggs Australian.
Charles Hakes Fort Lewis College1. Charles Hakes Fort Lewis College2.
HI Gas as Function of Environment When and where do galaxies stop accreting cool gas? How do they loose the cool gas? When do they stop forming stars?
Probing the field of Radio Astronomy with the SKA and the Hartebeesthoek Radio Observatory: An Engineer’s perspective Sunelle Otto Hartebeesthoek Radio.
HI in galaxies at intermediate redshifts Jayaram N Chengalur NCRA/TIFR Philip Lah (ANU) Frank Briggs (ANU) Matthew Colless (AAO) Roberto De Propris (CTIO)
HI from z ~ 0 – 1 with FAST D.J. Pisano West Virginia University NRAO.
SKA Science Measuring Variations in the Fundamental Constants with the SKA Steve Curran School of Physics School of Physics University of New South Wales.
What good are low frequencies? HI, neutral hydrogen, H 0, atomic hydrogen high redshifts and early times…. USS, GPS, … “enabling technologies” …multi-beaming,
The Evolution of Gas in Galaxies End of Thesis Colloquium Philip Lah.
The HI gas content of galaxies around Abell 370, a galaxy cluster at z = 0.37 International SKA Forum 2010 Philip Lah A New Golden Age for Radio Astronomy.
Measuring the Gas in Galaxies in the Distant Past Philip Lah Too late. Here comes the SKA.
Eric M. Wilcots University of Wisconsin-Madison.  How and when did galaxies accrete their gas?  Where and when did/do galaxies stop accreting gas? 
Multiwavelength Sky by NASA. Radio Continuum (408 MHz). Intensity of radio continuum emission from surveys with ground- based radio telescopes (Jodrell.
HI in Galaxies at Redshifts 0.1 to 1.0: Current and Future Observations Using Optical Redshifts for HI Coadding Melbourne 2008 Philip Lah.
Neutral Hydrogen Gas in Abell 370, a Galaxy Cluster at z = 0.37 NCRA 17 th July 2008 Philip Lah.
HI in Galaxies at Redshifts 0.1 to 1.0: Current and Future Observations Using Optical Redshifts for HI Coadding Deep Surveys of the Radio Universe with.
The Future of the Past Harvard University Astronomy 218 Concluding Lecture, May 4, 2000.
HI at moderate redshifts Philip Lah Science with MIRA workshop Research School of Astronomy & Astrophysics Mount Stromlo Observatory.
The Evolution of Stars and Gas in Galaxies: PhD Midterm Philip Lah A journey with noise and astrometry.
HI in galaxies from z = to z = 0.2 Thijs van der Hulst
Neutral Hydrogen Gas in Star Forming Galaxies at z=0.24 Philip Lah Frank Briggs (ANU) Jayaram Chengalur (NCRA) Matthew Colless (AAO) Roberto De Propris.
Neutral Hydrogen Gas in Star Forming Galaxies at z=0.24 HI Survival Through Cosmic Times Conference Philip Lah.
Susan CartwrightOur Evolving Universe1 Galaxy evolution n Why do galaxies come in such a wide variety of shapes and sizes? n How are they formed? n How.
Star Formation Rate and Neutral Gas Content as a Function of Redshift and Environment Collaborators: Mike Pracy, Jayaram Chengalur, Frank Briggs, Matthew.
Direct Measurement of a Magnetic Field at z=0.692 Art Wolfe Regina Jorgenson: IOA Tim Robishaw: UCB Carl Heiles:UCB Jason X. Prochaska:UCSC.
M 51. M 51 Galaxy merger simulation.
Galaxies Live in Clusters Hickson Fornax. Coma Virgo.
Active Galaxy Jets – An exhausting business Diana Worrall University of Bristol.
A hot topic: the 21cm line I Benedetta Ciardi MPA.
Nebular Astrophysics.
The Cosmic Evolution of Neutral Atomic Hydrogen Gas AAO Colloquium 5th February 2015 Philip Lah.
Cosmic magnetism ( KSP of the SKA) understand the origin and evolution of magnetism in the Galaxy, extragalactic objects, clusters and inter-galactic/-cluster.
Interaction in the NGC 3079 group Nebiha Shafi University of Witwatersrand and HartRAO Supervisors: Prof. Roy Booth (HartRAO) Dr. Raffaella Morganti Dr.
Imaging Compact Supermassive Binary Black Holes with VLBI G. B. Taylor (UNM), C. Rodriguez (UNM), R. T. Zavala (USNO) A. B. Peck (CfA), L. K. Pollack (UCSC),
Unravelling the formation and evolutionary histories of the most massive galaxies Ilani Loubser (Univ. of the Western Cape)
Lecture Outlines Astronomy Today 8th Edition Chaisson/McMillan © 2014 Pearson Education, Inc. Chapter 25.
Note that the following lectures include animations and PowerPoint effects such as fly-ins and transitions that require you to be in PowerPoint's Slide.
Lecture 18 : Weighing the Universe, and the need for dark matter Recap – Constraints on the baryon density parameter  B The importance of measuring the.
High energy Astrophysics Mat Page Mullard Space Science Lab, UCL 6. Jets and radio emission.
Magnetic fields in the Galaxy via Faraday effect: Future prospects with ASKAP and the SKA Lisa Harvey-Smith Collaborators: Bryan CSIRO SKA Project ScientistGaensler.
Faint Low Surface Brightness Galaxies in the Virgo Cluster Jonathan Davies, Sabina Sabatini and Sarah Roberts SAO September 2009.
Time domain science and LSST follow ‐ up in South Africa (+ SKA) Stephen Potter South African Astronomical Observatory.
ASTR112 The Galaxy Lecture 7 Prof. John Hearnshaw 11. The galactic nucleus and central bulge 11.1 Infrared observations (cont.) 11.2 Radio observations.
Radio Waves Interaction With Interstellar Matter
Structure Formation in the Universe Concentrate on: the origin of structure in the Universe How do we make progress?How do we make progress? What are the.
Galaxies with Active Nuclei Chapter 14:. Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus).  “active galactic.
The clustering of galaxies detected by neutral hydrogen emission Sean Passmoor Prof. Catherine Cress Collaborators Andreas Faltenbacher, Ando Ratsimbazafy.
Copyright © 2010 Pearson Education, Inc. Clicker Questions Chapter 14 The Milky Way Galaxy.
Radio Galaxies Part 3 Gas in Radio galaxies. Why gas in radio galaxies? Merger origin of radio galaxies. Evidence: mainly optical characteristics (tails,
C.Carilli, AUI Board October 2006 ISAC-run three year process: Quantified ‘experiments’ for future large area cm telescopes 50 chapters, 90 authors, 25%
Lyman Alpha Spheres from the First Stars observed in 21 cm Xuelei Chen (Beijing) Jordi Miralda Escudé (IEEC, Barcelona).
Introduction to Galaxies Robert Minchin. What is a galaxy?
Competitive Science with the WHT for Nearby Unresolved Galaxies Reynier Peletier Kapteyn Astronomical Institute Groningen.
Chapter 25 Galaxies and Dark Matter. 25.1Dark Matter in the Universe 25.2Galaxy Collisions 25.3Galaxy Formation and Evolution 25.4Black Holes in Galaxies.
What is EVLA? Giant steps to the SKA-high ParameterVLAEVLAFactor Point Source Sensitivity (1- , 12 hr.)10  Jy1  Jy 10 Maximum BW in each polarization0.1.
Cosmic Masers Chris Phillips CSIRO / ATNF. What is a Maser? Microwave Amplification by Stimulated Emission of Radiation Microwave version of a LASER Occur.
“Globular” Clusters: M15: A globular cluster containing about 1 million (old) stars. distance = 10,000 pc radius  25 pc “turn-off age”  12 billion years.
1 ASTRON is part of the Netherlands Organisation for Scientific Research (NWO) Netherlands Institute for Radio Astronomy Astronomy at ASTRON George Heald.
© 2017 Pearson Education, Inc.
Galaxy Formation and Evolution: Where we are and where we are going.
An Arecibo HI 21-cm Absorption Survey of Rich Abell Clusters
The Interstellar Medium
Galaxies With Active Nuclei
Galaxies With Active Nuclei
Presentation transcript:

MeerKAT Large Survey Projects SAAO Board, Roy Booth (SA SKA Project)

The MeerKAT Large Survey Proposals (MLS) MeerKAT (64 x 13.5m offset Gregorian antennas) will be the most powerful centimetre-wave radio telescope in the Southern Hemisphere until it is eventually merged with more (circa 180) SKA project 15m diameter antennas to form the SKA 1. MeerKAT will support scientific investigations within and beyond the MLS MLS proposals will occupy 70% of the observing time The other 30% is for PI proposals and ‘Targets of Opportunity’ at the Director’s discretion

MeerKAT Large Surveys Community response 3 22 countries

4 = place holder for VLBI with MeerKAT Includes magnetic fields in galaxies (polarization and Faraday rotation) and Faraday rotation)

1. HI (OH) Galaxy Surveys Distant Universe (LADUMA) z=1.4 (580 MHz) – Extended Chandra Deep Field South (Blythe, Baker and Holweda) ABSORPTION LINE SURVEY– HI (+OH) detection at high red- shifts and also investigation of magnetic fields (Zeeman splitting) and constancy of Fundamental constants as a function of z using OH lines and their different dependencies on the fine structure constant and the electron/proton mass ratio. Also millimetre and optical follow-up (Gupta and Srianand) Nearby galaxies of different types (MHONGOOSE) –Cosmic web, dark matter (de Blok) Galaxy Clustering (FORNAX cluster) Effects of galaxy-galaxy interaction, tidal stripping, galaxy formation in clusters,…. (Serra )

LADUMA Galaxies form from gas that cools and condenses in dark matter halos. In the local Universe (z < 0.5) HI is the easily detectable manifestation of this process (Guinevere Kaufman). Laduma will study H1 to z=1.2! High-z HI (even OH) in galaxies in a single field (ECDFS) in two phases (z= 0.58 and z> 1.2 (according to the receiver roll-out of MeerKAT). Goals Measurement of integrated HI masses in relation to environment, to halo mass, Stellar mass. HI emission v. absorption For the first time to investigate the HI galaxy content out to z=1.2 (Probably rely on optical red shifts – and may need more?)

LADUMA a deep HI survey to z=1.2 Mark Verheijen

HI Observations of the FORNAX Cluster PI Serra Fornax is the second most massive cluster within 20 Mpc form us and the largest cluster in the southern hemisphere. Its low X-ray luminosity makes it representative of the environment where most galaxies live. Furthermore, Fornax’ ongoing growth makes it an excellent laboratory for the study of structure formation. Ideally located for MeerKAT observation, it provides an excellent opportunity to study the assembly of clusters, the physics of the accretion and stripping of gas in galaxies falling in the cluster, and to probe for the first time the connection between these processes and the neutral medium in the cosmic web.

HST heritage image

Mhongoose - Galaxy Assembly & Evolution – de Blok

/tmp/PreviewPasteboardItems/NWONRF_deb lok.pdf

Follow-up to ‘THINGS’ survey with VLA Studying relatively local galaxies and the connection between star formation and HI dynamics and accretion Outer discs of galaxies and the cosmic web Comparison of Spitzer data, Relationship to molecular gas fn(radius)

The Velocity Field of M31 and the Dark Matter Radio observations of the neutral hydrogen line in nearby galaxies showed that the speed of rotation of the gas is constant far beyond the optical image. The optical image suggests that the galaxy must be embedded in a huge dark matter halo. No dark halo

HI Absorption lines – Gupta and Srianand Pks Z = Kanekar and Chengalur GMRT HI may be detected more easily in absorption against a background continuum source

GMRT 230 MHz z=5.2?  Continuum point source = 0.55 Jy  Noise limited spectra: s =5.5 mJy/channel  HI 21cm absorption at z=5.200? t = 4%, D v = 130 km/s N(HI) = 9e20 (T s /100K) cm^-2

Chile Goals 1) Blind search for 21cm and OH absorbers at z<1.8: using MHz frequency band(s). Detect more than ~600 intervening 21-cm absorbers: 20 times the number of absorbers known. 3) Measure the evolution of cold atomic and molecular gas at z<1.8: the z-range where most of the evolution in SFRD takes place. 4) Time variation of the fundamental constants of physics: using OH lines, and 21-cm and optical/UV absorption lines (SALT + VLT + ALMA). 5) Probe the magnetic field in absorbing galaxies: using rotation measure and Zeeman splitting. 6) Synergy with ALMA, EVLA, SALT, VLBA and VLT all the data will be public.

FUNDAMENTAL CONSTANTS Basic Idea: Measure the apparent redshifts of two spectral lines whose frequencies have different dependences on fundamental constants (eg OH lines) From the observed redshift difference determine rate of change of relevant constants (or get upper limits) Fine structure constant Electron/proto mass ratio Proton g-factor Rydberg constant

Frequencies and LTE line ratios F= MHz1 F= MHz5 F= MHz9 F= MHz1 In normal OH, spectra in all 4 lines give info on excitation conditions. Could be important for MeerKAT Hydroxyl (OH) The OH rotational line is split: First by an interaction between the electronic angular momentum and the molecular rotation Then, each energy level is split again through the interaction of the nuclear magnetic moment with the magnetic moment of the orbiting electron Different dependences on alpha and on the electron – proton mass ratio

OH 2  3/2 ground-state transitions  doubling: Interaction of electronic angular momentum with molecular rotation hfs splitting: Interaction of nuclear magnetic moment of with magnetic moment of orbiting electron  Different dependences on  and y = m e /m p Fundamental treatment:

CapeTown cm absorbers for the fundamental constant studies What is a good system for fundamental constant studies ? Gupta et al. 2009

Case of J (z=1.3603) CapeTown Case of J (z=1.3603) Compact at VLBI scales Rahmani et al Compact at VLBI scales

CapeTown Rahmani et al Discrepancies in the variation? of the Fine structure constant Rahmani et al used optical spectra taken with the UVES Echelle Spectrograph at the VLT and 21 cm absorption data from the GMRT

2. High frequency spectroscopy nb high frequency receiver 8 – 15 GHz 1.High-z CO (MESMER) – PI – Ian Heywood (MeerKAT Search for Molecules in the epoch of reionisation) CO is a surrogate for H 2 which has no dipole moment and so no rotational spectrum CO already detected in two galaxies at z (even greater) - and commonly at z=4 and less Evidence that molecular hydrogen more abundant than atomic hydrogen in the early Universe, where galaxies more tightly bound (pressure/gas density higher) How common is high-z CO? This study was one of the drivers for a high frequency band on MeerKAT

SDSS J : Gas detection z = 6.42 (t = 0.87 Gyr) L bol = L  SMBH ~ 3  10 9 M  M(H 2 ) ~ 2  M  VLA PdBI Fuel for Galaxy Formation Size ~ 5.5 kpc Radio-FIR SED follows star forming galaxy SFR ~ 3000 M  /yr Carilli et al. CO and dust detected at z=6.42, already close to EoR

Theory for HI and H2 in Galaxies Obreschkow et al., 2009, ApJ Properties of HI and H2 in a normal galaxy Molecular hydrogen/atomic hydrogen ratio depends on Pressure, which builds up towards the centre of normal galaxies

Three stage observational scheme: Stage 1: Target fields containing lensing clusters, (A370, A 1689 and MACS 2129) chosen because they have no bright radio sources) thereby taking advantage of the lensing magnification in source brightness, angular extents and source counts that lensing affords. (3 x 600 hrs) Sensitivity in a 1 MHz bandwidth is about 10 microjansky in 250 hrs Stage 2: High-z quasars and some blank fields (9 x 300 hrs) Stage 3: One square degree survey centred on a prominent field already targeted by other surveys eg ECDFS (250 x 8 hrs)

MeerGAL – High-frequency survey of the Milky Way Galaxy (and Magellanic Clouds) Mark Thompson and Sharmila Goedhart Unique to MeerKAT and another reason for GHz Stellar formation and evolution - HII Regions, Recombination lines and Galactic Rotation Curve, interstellar molecules, Astrobiology - new molecules, molecules of life…. MASERS throughout the Galaxy - astrometry follow-up with VLBI

Astrobiology at Long Wavelengths > 1 cm Not affected by dust Complex molecules have transitions at longer wavelengths “Waterhole” (1.4–1.7 GHz) Leakage emissions from extrasolar planets! Origins First Light Galaxy Evolution Astrobiology

3: Deep Continuum studies (Mightee) van der Heyden and Jarvis Long integrations of selected regions in order to reach micro-Jansky sensitivity levels Will integrate on the same field as Laduma Synergy with the wider field ASKAP-EMU survey Mightee is so sensitive that it is very likely to detect new types of radio sources – showing the way the radio galaxy population evolved

Approach to major radio surveys The wedding-cake approach

Diagram courtesy of Isabella Prandoni Limit of conventional radio-telescopes SKA pathfinders Current major 20cm surveys SKA pathfinders NVSS 75% of sky rms=450μJy EMU 75% of sky rms=10μJy

Current major 20cm surveys Diagram courtesy of Isabella Prandoni Limit of conventional radio-telescopes SKA pathfinders

– Pulsars Pulsar Timing (Bailes), Trapum (Stappers and Kramer) Pulsar timing – gravitational waves Pulsar timing – variations in period may indicate gravitational waves pervading the medium Pulsar Searches – looking for new types of Pulsar some switch on and off – why? how?

Pulsars are rotating neutron stars Mass 1.4 M o Radius10 km Surface – crystalline solid, density 10^6 gm/cc Outer core – solid with free neutrons Inner core – neutron superfluid, d=10^14 Popssible solid central core; Central density 10^15 g/cc

Pulsar size

Pulsar timing MeerKAT 4.5 times as sensitive as Parkes (Matthew Bailes, PI Pulsar timing at X-band)

High frequency Pulsar observations Exploration of Central region of the Galaxy to conduct precision Pulsar timing with the aim of detecting the gravitational wave background using an array of millisecond pulsars. Rigorously test General Relativity and alternative theories of gravity using the double pulsar and other relativistic binaries. determine the distribution of neutron star masses, precisely map the orbits of the binary pulsars to trace their origin and evolution, study pulsar planetary systems, determine the origin and evolution of the globular cluster pulsars. study the internal structure of neutron stars via glitch monitoring, explore the radio pulsar emission mechanism and its relation to gamma-ray and x-ray emission. understand the magnetars, determine a large number of pulsar parallaxes and proper motions, rigorously map the interstellar medium, study the single pulses of a large ensemble of pulsars, determine the pulsar birthrate and population and determine the true nature of the rotating radio transients (RRATs).

PULSARS and Tests of General Relativity and Search for Gravitational Waves Huge pulsar surveys will discover pulsar black hole binaries, providing direct tests of gravity in the strong field limit. Huge numbers of pulsars provide an array of very stable “clocks” which can be used to detect a background of grav waves.

ThunderKAT – Extreme Physics (Woudt and Fender) Slow radio transients (several seconds and longer in duration) are relatively rare. eg Supernovae, Novae and even more exotic objects. But rather few studies have been undertaken. Gamma ray bursts from AGN and other compact radio sources are observed occasionally, but have not been well studied or fully understood. ThunderKAT aims to monitor a wide field with MeerKAT in the hope of finding transient events. Other instruments will be ready to follow up on those events. The essence of the project is the high sensitivity of MeerKAT, a spigot from the correlator permanently connected to the transient detector system and the ability to marshal other instruments to follow through in the radio and other wavelengths. Optical follow-up is of great interest.

The way forward

The MeerKAT organization is anxious to ensure that the successful Survey Teams shall work with us to ensure a coherent approach to issues like Project Development, Special Software, Data Format (we propose VO compatibility), Team Organisation and Dynamics (working groups), Publication/Data Release Policy and Outreach. Large Survey Oversight Team set up to conduct regular (quarterly) meetings of PIs and request that the Project teams conduct annual meetings with our scientific/technical liaison personnel, Roy Booth and Justin Jonas (in the first instance), to report progress, problems and possible changes in scientific priorities as other projects progress. The project will adapt HR policy towards special postdocs and PhD positions in fields related to the accepted Large Survey Programmes, and request that a reciprocal policy is adopted by the team leaders. From Bernies letter to Successful PIs

Supporting the MLS Regular interactions with PIs Persuading surveys to set up working groups to interact directly with appropriate engineering teams – software (pipeline), digital (correlator)….system eng. (specs) Involvement of PIs in KAT-7 commissioning Annual MLS progress meetings with project reps.

ASKAP and Meerkat are different from conventional telescopes They will both be dominated by large survey projects Nobody will go to the telescope to observe Observations will be orchestrated by the Ops team - often two projects simultaneously Observers won’t reduce their data – It will all be reduced in real-time in a pipeline – Producing images, cubes, source catalogs., etc PIs will mine the data on the web – Using VO tools

Common scientific questions/requirements across the pathfinders Exploiting synergies G. Kaufman The balance between wide/shallow (ASKAP) and narrow/deep (MeerKAT) surveys and cooperation on location of fields Ancillary data – familiarity with optical, IR and other data, sources, spectra, etc Critical tools – Pipelines, source extraction, (source extraction in the presence of a strong source - peeling), polarisation measurement, data analysis tools (eg automatic extraction of rotation curves using model fitting and other techniques), non circular motions, radial flow analysis Tools for interpretation – simulations of galaxy/AGN systems, source counts, source evolution, constraints by large scale structure (cosmic web), predictions of source/galaxy populations in cosmological volumes, N-body simulations

Moving forward Networking among the pathfinder survey groups Using existing telescopes (eg KAT-7 but also other telescopes) to obtain pilot data sets that can be used by everyone for tuning source extraction algorithms, data analysis pipelines… A forum for sharing expertise in software – perhaps leading to more uniformity across the surveys Public data base of simulations Data bases of ancillary data- Optical/IR imaging, spectroscopy, X-ray data,… Some of these collaborations already exist in eg the Pulsar community but we should become part of them, and participate in setting up others