oct 16, 2008, sfig, zhiyu zhang, seminar 2008 introduction of radio interferometry and the evla...
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Oct 16, 2008, SFIG, Zhiyu Zhang, Seminar 2008
Introduction of Radio Interferometry
and the EVLA
Zhiyu Zhang
Oct 16, 2008, SFIG, Zhiyu Zhang
Introduction of interferometers Fundamental of interferometry
Next generation radio interferometers
Introduction of E-VLA
Science cases
Summary
OutlineOutline
Oct 16, 2008, SFIG, Zhiyu Zhang
Introduction of interferometers
Real time
m–cm: WSRT, GMRT, VLA, ATCA, etc.
Mm: CARMA, PdBI, etc.
Sub-mm: SMA etc.
VLBI
E-MERLIN, EVN, VLBA, LBA, Space-VLBI(VSOP) etc.
Optical: VLT-I, and?
Oct 16, 2008, SFIG, Zhiyu Zhang
Advantage and shortcoming
Best resolution – VLBI ~10-6 arcsec, Much better than single dish telescopes at the same band!!!
Stable -- even part of it can work.
Flat baseline – much better than single dish
3-D data cube -- 4-D information. position, intensity, and spectral line.
Tracing position – Spacecrafts, asteroid, etc.
Rapid response – Pulsar
Very long time integration – more than one day, can be thousands of hours____________________________________
Missing flux -- can be partly adjusted
Expensive -- cost for correlators
Deconvolution algorithm -- fast Fourier transition, not only one solution
Complicated calibration – phase, flux, bandpass etc.
Data reduction – hard to study
Oct 16, 2008, SFIG, Zhiyu Zhang
FundamentalFundamental
Angular resolution ~ λ/B & frequency
Resolution -- depends on shortest & longest baseline
Field of view (FOV) -- equal to single dish main beam
UV-coverage -- depends on earth rotation, and configuration of antennas. interpolating & imaging quality
Antenna configuration – beam response and better UV-coverage
Phase Calibration -- calibration for position
Bandpass calibration -- calibration for spectra
Flux calibration -- calibration for flux
De-convolve algorithm -- CLEAN, MEM, Hybrid, etc.
Oct 16, 2008, SFIG, Zhiyu Zhang
DSingle dish: = /D
B
Interferometer: = /B
Scheme
Oct 16, 2008, SFIG, Zhiyu Zhang
combine signals from two antennas separated by baseline vector b in a correlator; each sample is one “visibility”
• each visibility is a value of the spatial coherence function V (b) at coordinates u and v obtain sky brightness distribution by Fourier inversion:
s
b
Visibility
Oct 16, 2008, SFIG, Zhiyu Zhang
UV-Coverage
ALMA snapshot
Central hole
Oct 16, 2008, SFIG, Zhiyu Zhang
Clean Imaging
Weighting
Self-calibration
Resampling
3D-2D
Algorithm:
CLEAN
MEM
Hybrid
Oct 16, 2008, SFIG, Zhiyu Zhang
Introduction of a few of next generation interferometers
ATA
EVLA
ALMA
LOFAR
SKA
350x 6m64 x 12m
25000 elements
one square kilometer
Oct 16, 2008, SFIG, Zhiyu Zhang
Introduction of the VLA
Built 1970’s, dedicated 1980,27 x 25m diameter antennasTwo-dimensional 3-armed array designFour scaled configurations, maximum baselines 35, 10, 3.5, 1.0 Km. Eight bands centered at 0.074, 0.327, 1.4, 4.6, 8.4, 15, 23, 45 GHz100 MHz total IF bandwidth per polarizationFull polarization in continuum modes.Digital correlator provides up to 512 total channels – but only 16 at maximum
bandwidth.
VLA in D-configuration(1 km maximum baseline)
Oct 16, 2008, SFIG, Zhiyu Zhang
Introduction of the EVLA
Sensitivity: Continuum sensitivity improvement over the VLA by factors of 5 to 20, to give point-source sensitivity better than 1 microJy between 2 and 40 GHz.
Frequency Accessibility: Operation at any frequency between 1.0 and 50 GHz, with up to 8 GHz bandwidth per polarization.
Spectral Capability: Full polarization (8 GHz bandwidth per polarization), with a minimum of 16,384 channels, frequency resolution to 1 Hz, and 128 independently tunable sub-bands.
Resolution: Angular resolution up to 200 / (frequency in GHz) milliarcseconds with tens of Kelvin brightness temperature sensitivity at full resolution.
Low-Brightness Capability: Fast, high fidelity imaging of extended low-brightness emission with tens of arcseond resolution and microKelvin brightness sensitivity.
Imaging Capability: Spatial dynamic range greater than 106, frequency dynamic range greater than 105, image field of view greater than 109 with full spatial frequency samplng.
Operations: Dynamic scheduling, based on weather, array configuration, and science requirements. "Default" images automatically produced, with all data products archived.
Oct 16, 2008, SFIG, Zhiyu Zhang
Ultrasensitive Array
New Mexico Array
VLA
by 2012
Two Phases
Ten new antennas
Range up to 250 Km from EVLA
+WIDAR
Wideband Interferometric Digital ARchitecture
Receivers
PHASE I
PHASE IIProposed
Oct 16, 2008, SFIG, Zhiyu Zhang
EVLA Phase I - Key Science Examples Measuring the three-dimensional structure of the Sun's magnetic field Mapping the changing structure of the dynamic heliosphere Measuring the rotation speed of asteroids Observing ambipolar diffusion and thermal jet motions in young stellar objects Measuring three-dimensional motions of ionized gas and stars in the centre of the Galaxy Mapping the magnetic fields in individual galaxy clusters Conducting unbiased searches for redshifted atomic and molecular absorption Looking through the enshrouding dust to image the formation of high-redshift galaxies Disentangling starburst from black hole activity in the early universe Providing direct size and expansion estimates for up to 100 gamma-ray bursts every year
Main Science Projects
EVLA Phase II - Key Science Examples AU-scale imaging of local star forming regions and proto-planetary disks Resolving the dusty cores of galaxies to distinguish star formation from black hole accretion Imaging at the highest resolution at any wavelength of the earliest galaxies (z~30) Imaging of galaxy clusters with 50 kpc or better resolutions at arbitrary redshifts Imaging of thermal sources at milliarcsecond scales Resolving individual compact HII regions and supernova remnants in external galaxies as distant as M82 Tying together the optical and radio reference frames with sub-milliarcsecond precision Measuring accurate parallax distances and proper motions for hundreds of pulsars as distant as the Galactic Center Providing 50 pc or better resolution for galaxies at any redshift Monitoring and imaging the full evolution of the radio emission associated with X-ray and other transients
Oct 16, 2008, SFIG, Zhiyu Zhang
Resolution vs. Frequency VLA vs. EVLAA key EVLA requirement is continuous frequency coverage from 1 to 50 GHz.This will be met with 8 frequency bands:
Two existing (K, Q)Four replaced (L, C, X, U)Two new (S, A)
Existing meter-wavelength bands (P, 4) retained with no changes. Blue areas show existing coverage. Green areas show new coverage.
Oct 16, 2008, SFIG, Zhiyu Zhang
Resolution vs. Frequency VLA vs. EVLA
Oct 16, 2008, SFIG, Zhiyu Zhang
NOISE regimes
Oct 16, 2008, SFIG, Zhiyu Zhang
Parameter VLA EVLA FactorPoint Source Sensitivity (1-, 12 hours) 10 Jy 1 Jy 10
Maximum BW in each polarization 0.1 GHz 8 GHz 80
Frequency channels at max. bandwidth 16 16,384 1024
Maximum number of frequency channels 512 4,194,304 8192
Coarsest frequency resolution 50 MHz 2 MHz 25
Finest frequency resolution 381 Hz 0.12 Hz 3180
(Log) Frequency Coverage (1 – 50 GHz) 22% 100% 5
Sensitivity, Bandwidth & Frequency resolution
Oct 16, 2008, SFIG, Zhiyu Zhang
1δ, 12 h integrationSensitivity
Oct 16, 2008, SFIG, Zhiyu Zhang
Continuum Sensitivity vs. Frequency
VLA
EVLA
ALMA
Oct 16, 2008, SFIG, Zhiyu Zhang
SKA will have
A sensitivity
of hundred times
of the VLA
Arp 220 as a template of High Z galaxies
Oct 16, 2008, SFIG, Zhiyu Zhang
4 P L C X U K Q
F (GHz) 0.073-0.0745 0.3-0.34 1.34-1.73 4.5-5.0 8.0-8.8 14.4-15.4 22-24 40-50
(cm) 400 90 20 6 3.6 2 1.3 0.7
(′) 600 150 30 9 5.4 3 2 1
(″) 24 6 1.4 0.4 0.24 0.14 0.08 0.05
Flx(mJy, 10 min)
150 1.4 0.056 0.054 0.045 0.019 0.10 0.25
T(K) 103-104 150-180 37-75 44 34 110 50-190 90-140
Full Band Coverage 1 ‘continuum’ (maximum sensitivity) observations
2 spectral line surveys
Oct 16, 2008, SFIG, Zhiyu Zhang
FIRSTA. Faint Images of the Radio Sky at
Twenty-centimetersB. Flux limit = 1mJyC. Resolution limit = 5″D. ~90/sq degreeE. Coincide with SDSS
NVSS (1993.9-1996.10)A. NRAO VLA Sky Survey B. Configuration D and DnCC. F = 1.4 GHz
.D >-40°E. Completeness limit ~ 2.5 mJyF. Resolution ~ 45″G. 1.8 106 sources
Survey Speed
EVLAVLA
Oct 16, 2008, SFIG, Zhiyu Zhang
Arp 220, Z=8?High Z CO survey
Oct 16, 2008, SFIG, Zhiyu Zhang
K-band spectra, in Massive SFR, One tuning pair (4 pairs totally)
Oct 16, 2008, SFIG, Zhiyu Zhang
64 Spectral Lines, with Full Polarization, and different spectral resolution
with 4-bit Re-Quantization
1. 18.6 - 20.6 GHz which covers 3 RRL + 1 Mol, 12 sub-band pairs (SBP) free
2. 20.6 - 22.6 GHz which covers 2 RRL + 3 Mol, 11 SBP free
3. 22.6 - 24.6 GHz which covers 2 RRL + 14 Mol, all SBP used
4. 24.6 - 26.6 GHz which covers 1 RRL + 14 Mol, 1 SBP free
24 SBP
40 SBPContinuum
Spectra
Oct 16, 2008, SFIG, Zhiyu Zhang
Ideas
1. super-fine spectral resolution observation towards molecular clouds – get the information of each clump. ( High performance in spectral observation)
2. RRL observation – Broad line region in AGNs? (High sensitivity and very broad bandwidth, and later high resolution to resolve)
3. H2CO maser survey in the Galaxy? (Hi sensitivity, fast survey speed, without confusion from surrounding absorption)
4. Weak molecular absorption lines towards continuum sources like SNR or quasar, as dense gas tracer.
5. I am still thinking about some interesting attempts.
Oct 16, 2008, SFIG, Zhiyu Zhang
Thank You!
Oct 16, 2008, SFIG, Zhiyu Zhang
Backup Slides
Oct 16, 2008, SFIG, Zhiyu Zhang
Now w points to the source, u to the east, and v toward the North.The direction cosines l and m ( on the celestial sphere plane) increase to the east and the north respectively.
UV-plane
Oct 16, 2008, SFIG, Zhiyu Zhang
Assume small frequency width (Δν) and no motion of the source.Now consider radiation from a small solid angle dΩ from direction S
Stationary, Monochromatic, Two element Interferometer
It is multiply but not plus because of
lower noise.
Oct 16, 2008, SFIG, Zhiyu Zhang
Making a SIN Correlator
Oct 16, 2008, SFIG, Zhiyu Zhang
Adding a time delay Change the spatial resolution to the resolution of time (much easier to handle)
Oct 16, 2008, SFIG, Zhiyu Zhang
Visibility
We now define a complex function, V, from the two independent correlator outputs:
This gives us a beautiful and useful relationship between the source brightness, and the response of an interferometer:
Oct 16, 2008, SFIG, Zhiyu Zhang
A Schematic Illustration
1 The correlator can be thought of ‘casting’ a sinusoidal coherencepattern, of angular scaleλ/b radians, onto the sky.
2 The correlator multiplies the source brightness by this coherence pattern, and integrates (sums) the result over the sky.
3 Fringe separation set by baseline length and wavelength
Long baseline gives close-packed fringes.
Short baseline gives widely-separated fringes.
Oct 16, 2008, SFIG, Zhiyu Zhang
Can’t be sampled, missing flux
Oct 16, 2008, SFIG, Zhiyu Zhang
UV Coverage of the VLA/EVLA
Missing flux
Oct 16, 2008, SFIG, Zhiyu Zhang
Oct 16, 2008, SFIG, Zhiyu Zhang
Dirty beam
Oct 16, 2008, SFIG, Zhiyu Zhang
Software
Newstar :WSRT, Nobeyama, etc.
GILDAS(MIRA) :IRAM PdBI
MIRIAD :WSRT, ATCA, CARMA, SMA etc.
AIPS :VLA, VLBA, etc.
MIR :SMA
AIPS++ => CASA :ALMA, EVLA, PdBI, etc.
Uniform, convenience, good at imaging
Powerful, complicated, good at calibration and
specific usage
Powerful, Uniform, Convenience,
Still in programming
Oct 16, 2008, SFIG, Zhiyu Zhang
H7
1
H7
0
H6
9
H6
8
H6
7
H6
6
H6
5
H6
4
H6
3
H6
2
K-band spectra line excitation temperature?