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The Dynamic Radio Sky and Future Instruments
Jim Cordes Cornell University
AAS MeetingNashville
28 May 2003
Dynamic Radio Sky
• We know enough about the DRS to know that there is a great deal yet to be discovered
• c.f. the high energy universe, optical, etc.• What is in the DRS?• What are the prospects for new discoveries?
Astrophysical parameters Extrinsic effects RFI
• Instruments & surveys that will reveal the DRS
TRANSIENT SOURCES TRANSIENT SOURCES Sky Surveys:Sky Surveys:The X-and-The X-and--ray skies have been monitored highly successfully -ray skies have been monitored highly successfully with wide FOV detectors with wide FOV detectors (e.g. RXTE/ASM, CGRO/BATSE).
Neutrino/gravitational wave detectors are ‘all sky.’Neutrino/gravitational wave detectors are ‘all sky.’
Optical transient surveys (ROTSE, RAPTOR, LSST) are/will Optical transient surveys (ROTSE, RAPTOR, LSST) are/will revolutionalize our knowledge of the optical transient sky and revolutionalize our knowledge of the optical transient sky and will drive the trend toward data mining of will drive the trend toward data mining of » » petabyte databases.petabyte databases.
The transient radio sky (e.g. t < 1 month) is largely unexplored.The transient radio sky (e.g. t < 1 month) is largely unexplored.
New objects/phenomena are likely to be discovered as well as New objects/phenomena are likely to be discovered as well as extreme cases in predictable classes of objects.extreme cases in predictable classes of objects.
Ingredients for transient detection
AT needs to be “large”
A = collecting area
= solid angle covered (instantaneous FOV)
T = time per sky position
Issue: to dwell (stare), or tile the sky, or be triggered?
Successes in transient astronomy
RXTE/ASM
VelaROTSE
RAPTOR
Why is the Dynamic Radio Sky Largely Uncharted?
• Large collecting areas, A, needed for sensitivity• Typically A is small enough that telescope
throughput is small• Telescope time is expensive so dwell times are short• Sources cover a wide range of time scale and sky
density
insufficient sky and temporal coverage
Giant pulse from the Crab pulsar
S ~ 160 x Crab Nebula
~ 200 kJy
Detectable to ~ 1.5 Mpc with Arecibo
Arecibo
2-ns giant pulses from the Crab: (Hankins et al. 2003)
Giant Pulses seen from B0540-69 in LMC (Johnston & Romani 2003)
Giant pulses are the fastest known transients
• Giant pulses from Crab detectable to ~1.5 Mpc with Arecibo @ 1/hour
• 2-ns wide `nano-Giant pulses’ identified from Crab (Hankins et al. 2003)
• GPs seen from Crab clone in LMC (B0540-69) by Johnston & Romani (2003) w/ similar intrinsic amplitude
• GPs from two millisecond pulsars• Radio GPs in pulse components also
seen in X-rays• GP-emitting objects have ~ same B
fields at their light cylinders
Nano-giant pulses (Hankins et al. 2003)
Arecibo
5 GHz
0.5 GHz bw
coherent dedispersion
STARE 611 MHz 3-station radio transient detector (Katz, Hewitt, Corey, Moore 2003)
Solar Radio Bursts
GRB 980519 variability (Frail et al. 2000)
Interstellar scintillations
TRANSIENT SOURCES TRANSIENT SOURCES TARGET OBJECTS: TARGET OBJECTS:
• Atmospheric/lunar pulses from neutrinos & cosmic rays
• Accretion disk transients (NS, blackholes)• Neutron star magnetospheres• Supernovae• Gamma-ray burst sources• Brown dwarf flares (astro-ph/0102301)• Planetary magnetospheres & atmospheres• Maser spikes• ETI
TRANSIENT SOURCES TRANSIENT SOURCES TARGET PROCESSES:TARGET PROCESSES:
• Intrinsic:incoherent:
( inverse Compton brightness limit)coherent: (virtually no limit)continuum: low frequencies favored
spectral line: masers
• Extrinsic:scintillationmaser-maser amplificationgravitational lensingabsorption events
Phase Space for Transients: SpkD2 vs. W
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
W = light travel time
brightness temperature:
SpkD2
Tb = ------------- 2k (W)2
Phase Space for Transients: SpkD2 vs. W
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
Lines of constant brightness temperature
Phase Space for Transients: SpkD2 vs. W
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
Solar system
+
local galactic sources
Phase Space for Transients: SpkD2 vs. W
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
OH masers
+
Pulsars (including giant pulses)
Phase Space for Transients: SpkD2 vs. W
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
Cosmological sources:
AGNs (including IDV sources)
+
GRB afterglows
Phase Space for Transients: SpkD2 vs. W
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
Phase Space for Transients: SpkD2 vs. W
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
Interstellar scintillations = apparent fast variations of IDVs & GRBs
New instruments can cover this phase space
W
W
Pulse
Process
Spk
log
Sp
kD
2
log W
Exploring the Transient Radio Sky:Striving for large AT
• Pilot observations: Arecibo: single pixel and multibeam (ALFA) STARE and similar multisite arrays GBT: single pixel and multibeam arrays ATA: 2.5 deg FOV, ~8 array beams EVLA (wideband, high sensitivity & spatial resolution)
• LOFAR: low frequencies (< 240 MHz)• SKA: broad frequency range (0.15 to 25 GHz)
Giant pulses from M33Arecibo observations
(Maura Mclaughlin & Cordes, submitted to ApJ, astro-ph
Galactic Center TransientsVLA 0.33 GHz
Hyman et al. 2002
Exploring the Transient Radio Sky:Covering the Sky
• Staring vs. mosaicing (tiling)?• Radio sky needs both;
Fast transients: too fast to raster scan the sky (< hours to months) (e.g. GPs)
Slower transients: raster scan (e.g. for objects showing radio only) trigger from other wide-field instruments (GRB
afterglows)
TRANSIENT SOURCES TRANSIENT SOURCES Sure detectionsSure detections::
• Analogs to giant pulses from the Crab pulsar out to ~5 – 10 Mpc
• Flares from brown dwarfs out to at least 100 pc.
• GRB afterglows to 1 µJy in 10 hours at 10 .
PossibilitiesPossibilities::
• -ray quiet bursts and afterglows?-ray quiet bursts and afterglows?
• Intermittent ETI signals?Intermittent ETI signals?
• Planetary flares?Planetary flares?
Isolated pulsarRe-ignition of pulsar action in mergers?
Hansen & Lyutikov 2000
RFI Editing in the f-t planeRFI dynamic spectra (from AO monitoring program)
Dynamic spectrum of pulsar scintillation
Working Around Radio Frequency Interference
• Single-dish/single-pixel transient detection:• Very difficult to separate terrestrial & astrophysical
transients (significant overlap in signal parameter space)
• Multiple beam systems (Parkes, Arecibo, the GBT):• Simultaneous on/offs partial discrimination
Multiple site systems (a la LIGO, PHOENIX)• Very powerful filtering of RFI that is site specific or
delayed or Doppler shifted between sites
LOFAR = Low Frequency Array
Stations of dipoles
30 to 240 MHz
Large AT
Optimal for coherent continuum transients
SKA = Square Kilometer Array SKA = Square Kilometer Array
Current ConceptsCurrent Concepts
China KARSTChina KARST
Canadian Canadian aerostataerostat
US Large NUS Large N
Australian Australian Luneburg Luneburg LensesLenses
Dutch fixed Dutch fixed planar arrayplanar array
(cf. Allen Telescope Array,
Extended VLA)
(cf. LOFAR = Low Freqency Array)
Current Baseline SpecificationsParameter Design Goal Comments Sensitivity A/T = 2 x 104 m2 / K 20x Arecibo, 75x VLA Surface brightness 1K at 0.1 arcsec (cont) Point sources 0.5 Jy 10 in 1 day, 100 MHz Frequency range 0.15 – 22 GHz Redshift coverage Z < 8.5 HI,
Z > 4.2 CO (1 0)
L* galaxies Zmax ~ 2 HI, ~ 20 CO FOV (imaging) 1 degree2 at 1.4 GHz Multibeams > 100 Ang. Resolution 40 mas at 1.4 GHz VLBI: SKA enables all-sky
phase referencing Pixels 108 Instantaneous bandwidth
20% at high frequencies
Spectra channels 104 Image Dynamic Range
106 at 1.4 GHz
Polarization isolation
-40 dB
Methods with LOFAR & SKAMethods with LOFAR & SKA
I. Target individual objects
II. Blind Surveys: trade FOV against gain by multiplexing SKA into subarrays.
III. Allow rapid response to triggers
IV. Exploit coincidence tests to ferret out RFI, use multiple beams.
Primary beam & station Primary beam & station synthesized beamssynthesized beams
Station subarrays for Station subarrays for larger FOVlarger FOV
One station of many in SKAOne station of many in SKA
Blind Surveys with SKA
• Number of pixels needed to cover FOV:Npix~(bmax/D)2 ~104-109
• Number of operationsNops~ petaops/s
• Post processing per beam:e.g. standard pulsar periodicity analysis
Summary Transient science is unexplored territory for radio astronomy:
New looks at known sources Entirely new classes of sources: LOFAR will survey transients at f < 240 MHz; SKA for 0.15 GHz < f < 25 GHz (or more)
Implications for SKA design: Rapid imaging/mosaicing of sky (days) Large instantaneous FOV desired for short time scales (e.g.
hemispheric). US Plan: Subarrays to allow coincidence tests and maximal
sky coverage. Versatile imaging/beamforming/signal processing modes.
Similar implications for pulsar science
Radio Pulsars
• ~1400 known (doubled by Parkes MB)• ~100 millisecond pulsars• 2 to 3 with planets
• ~5 NS-NS binaries (Porb > 8 hr)
• MSPs have exceedingly stable spins, suitable for seeking gravitational wave perturbations
Why more pulsars?• Extreme Pulsars:
• P < 1 ms P > 8 sec
• Porb < hours B > 1013 G (link to magnetars?)
• V > 1000 km s-1
• NS-NS & NS-BH binaries
• Population & Stellar Evolution Issues
• The high-energy connection (e.g. GLAST)
• Physics payoff (GR, Gwaves, EOS, LIGO, GRBs…)
• Serendipity (strange stars, transient sources)
• New instruments (AO, GBT, LOFAR, SKA) will dramatically increase the volume searched (galactic & extragalactic)
Parkes MB Feeds
Parkes MB Feeds
ALFA Science Goals: Massive Surveys
Drift scan surveys (14 sec across 3.5 arcmin)
Deep Galactic plane survey (GPS) (5-10min, |b| < 5 deg, 30 < l < 80 + anticenter)
Medium latitude surveys ( 5 < |b| < 25 deg)
Targeted: globular clusters, high EM/DM HII regions, SNRs, Galactic chimneys, M33, X/ -ray selected objects
(long dwell times, up to 2.5 hr)
Surveys Surveys with Parkes, with Parkes, Arecibo & Arecibo & GBT.GBT.
Simulated & Simulated & actualactual
Yield ~ 1000 Yield ~ 1000 pulsars.pulsars.
ALFA Surveys at Arecibo• ALFA surveys can be viewed as part of a long-
term, grander effort (“Full Galactic Census”) (LOFAR, SKA, )
• RFI mitigation required and provides general purpose tools
• Data & data products = long term resources data management policy & resources~ 1 petabyte of survey raw data~ 1 petabyte of data products
• Exploit telescope time fully (transients, piggybacking)
SKA pulsar SKA pulsar surveysurvey
600 s per 600 s per beambeam
~10~1044 psr’s psr’s