data analysis in the radio - welcome to scippscipp.ucsc.edu/~tesla/emma_radiodatalec.pdf ·...
TRANSCRIPT
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Data Analysis in the Radio
Emma Storm
Astr 257: Modern Astronomical Techniques
May 28th, 2013
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Radio Data Analysis
interferometers measure antenna gains (voltages)
antenna gains are related to sky brightness via fourier transforms
only have access to raw, uncalibrated data
need to manually calibrate
image processing depends on science goals
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The VLA
VLA → EVLA → JVLA
27 25m-diametertelescopes (351baselines!)
4 configurations(A>B>C>D)
frequency range: 1-50GHz in 8 bands(L,S,C,X,Ku,K,Ka,Q)
Image courtesy of NRAO/AUI
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Interferometry Basics
Interferometers measureVisibility Functions
◮ correlated antennagains for each baseline(antenna pair)
◮ reported as a complexnumber: phase andamplitude at a givenposition in (u,v) space:
◮ u = bxλ, v =
byλ
From ERA online course (see references).
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Interferometry Basics
Astronomers wantBrightnessDistributions
◮ Iν(l,m), where◮ l = sinθx, m = sinθy
From ERA online course (see references).
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Interferometry Basics
How to get from Visibilities to Brightness: Fourier Transform!
(u,v) plane ↔ (l,m) plane
V (u, v) =∫Iν(l,m)e2πi(ul+vm)dldm
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VLA Basics
synthesized beam: θsb ∼λ
bmax
◮ 1.5 GHz (L), A config: 1.3”◮ 1.5 GHz (L), D config: 46”
primary beam: θpb ∼λD
◮ 1.5 GHz (L): 1700”
largest angular size: θLAS ∼ λbmin
◮ 1.5 GHz (L), A config: 36”◮ 1.5 GHz (L), D config: 970”
Sensitivity? Exposure Calculator
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VLA Exposure Calculator
theoretical thermal noise:
σth = SEFD
ηc√
npolN(N−1)tint∆ν
◮ ηc: correlator efficiency (>0.92for VLA)
◮ npol: number of polarizations= 2
◮ N: number of antennas◮ tint: total time on source◮ ∆ν: bandwidth in Hz◮ SEFD: system equivalent flux
density = flux density of aradio source that doublessystem temp
◮ See OSS for VLA SEFDs science.nrao.edu/facilities/vla/caltools/exposure
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Getting NRAO telescope data
for VLA, GBT, VLBA, ALMA
JVLA data sets are huge! 10s to100s of GB
Data Analysis Tools:◮ CASA: measurement sets◮ AIPS: fits files
NRAO Archive page:archive.nrao.edu/archive/advquery.jsp
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CASA: Common Astronomy Software Applications
new(ish): for JVLA and ALMA
The Measurement Set: series of binary tables
C++ tools bundled under a python interface:◮ can run interactively via ipython interface◮ can run non-interactively via python scripts
see CASA tutorials and cookbooks via nrao website
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Data Reduction
Look at your data!
Lots of manual flagging, calibration, hand tuning of images
General Steps:1 Initial flagging, smoothing2 A priori calibration3 Initial Calibration4 More flagging5 Calibration Round 26 More flagging and calibration, if needed7 Apply the Calibration8 Imaging: highly iterative9 Self Calibration?10 More imaging (and/or flagging and/or calibrating and/or
imaging...)
New: VLA pipeline (only for HF continuum observations)◮ science.nrao.edu/facilities/vla/data-processing/pipeline
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Calibrators in Observations
Flux Calibrator◮ strong, steady source
with known flux
Bandpass, Phase, GainCalibrators
◮ nearby target, scansinterspersed with thoseof target
◮ LF: ∼ 10 or more minscans
◮ HF: ∼ 1 min scans List of observation scans.
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Data Reduction: Visibility PlaneInitial Look and A Priori Calibration
Look to observing log forantenna issues to flagimmediately
Calibration of antenna positions,antenna gain vs elevation,weather (opacity) Antenna Positions.
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Data Reduction: Visibility PlaneLow Frequency Issue: Radio Frequency Interference (RFI)
RFI from humanswipes out largefrequency bandsin LFobservations
dealt with bysmoothing data,autoflagging tools
Badly RFI affected data.
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Data Reduction: Visibility PlaneHigh Frequency Issue: Rapid Phase Variations
atmosphericturbulence causeschanges in phaseover shorttimescales
dealt with byobserving phasecalibrator in shortintervals, carefulphase calibration
Phase variations in HF data. From IRC+10216 tutorial,casaguides.nrao.edu
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Data Reduction: Visibility PlaneBandpass, Gain, Flux Calibration
bandpass shape:amp and phase vsfrequency perantenna
antenna gain:amp and phase vstime per antenna
flux: scale flux oftarget relative toflux calibrator
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.0350.0400.0450.0500.0550.0600.065
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea01'
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.040
0.045
0.050
0.055
0.060
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea02'
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.040
0.045
0.050
0.055
0.060
0.065
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea03'
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.035
0.040
0.045
0.050
0.055
0.060
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea04'
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.040
0.045
0.050
0.055
0.060
0.065
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea05'
0.0 0.2 0.4 0.6 0.8 1.0Frequency (MHz)
0.00.20.40.60.81.0
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea06'
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.025
0.030
0.035
0.040
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea07'
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.040
0.045
0.050
0.055
0.060
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea08'
1300 1320 1340 1360 1380 1400Frequency (MHz)
0.040
0.045
0.050
0.055
0.060
0.065
0.070
Gai
n Am
plitu
de
B table: A2319Cspw0_B1.cal Antenna='ea09'
Bandpass shape for first 9 antennas.
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Data Reduction: Image PlaneCLEAN Algorithm
FT of visibility = source map convolved with psf (“dirty map”)
Clean task takes care of this, assumes source map is collection ofpoint sources
CLEAN Algorithm:1 deconvolves source map from psf map (leftover: “residual map”)2 finds highest peak in residuals3 subtracts out some percentage of peak4 adds the location and subtracted amplitude to a “model map” +
clean component list5 iterate over hundreds to thousands components...6 add back clean components to residuals, convolve with weighted
“clean” beam
Extended emission? – options to deal with this (e.g. boxes,multiscale cleaning...)
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Data Reduction: Image PlaneDirty Image
No clean components.
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Data Reduction: Image PlaneInteractive Cleaning
Residuals after 1000 clean components.
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Data Reduction: Image PlaneMasking
Residuals with masks on point sources.
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Data Reduction: Image PlaneWhen to Stop
set cleaningthreshold to somemultiple oftheoretical rmsnoise
interactively cleanuntil the imagelooks good! (e.g.,point sourcesappear to becleaned down tobackground noiselevel)
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Data Reduction: Image PlaneImage Quality
flux scale (doyour fluxes matchthose from e.g.,NVSS?)
rms noise nearsources and faraway
dynamic range:maximum fluxover rms noise
◮ JVLA datacapable ofdynamic rangein thethousands
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Data Reduction: Image Plane → Visiblity PlaneSelf Calibration
re-calibrate antenna gain using target itself, rather than gaincalibrator
if self-cal increases dynamic range, good!
typically requires many iterations
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Data Reduction: Image PlaneImage Quality: Patterns in the Residuals
residuals shouldbe random!
think in fourierspace
PSF artifacts around point sources, due to imperfect UV coverage.Not much you can do.
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Data Reduction: Image PlaneImage Quality: PSF Shape
PSF for previous image. Lots of structure!
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Data Reduction: Image Plane → Visibility PlaneImage Quality: Patterns in the Residuals
some artifactsrequire going backto visiblity plane
more flagging,etc.
Stripes, due to bad baseline or antenna, or RFI. Can remove this bygoing back to visiblity data.
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Data Reduction: Image PlaneFancier Options: Mosaicing
Multiple pointings put together into one image.
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Data Reduction: Image PlanePrimary Beam Correction
Primary beam corrected. Flux weighted based on primary beam shape.
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Data Reduction: Image PlaneMore Options
Wide Field Clean◮ baselines are not really in 2D plane◮ Wide Field clean takes 3D nature of baselines into account◮ can reduce artifacts far from center of primary beam
Multifrequency Clean◮ simultaneously images and fits for instrinsic source spectrum◮ useful for wide band observations (e.g. >few hundred MHz
bandwidth)
Multiscale Clean◮ for known extended emission◮ no set method, need to play around◮ good starting point: set scales to point source, 2-3x synthesized
beam, 2-3x expected extended emission sizes
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Data Reduction: Image PlaneFinalizing the Image
lots of image manipulation tools: add, subtract, scale, makecontours, etc
export to fits format for manipulation in e.g., ds9
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Data Reduction: Image PlaneCase Study: Imaging the halo of A2319
Clean point sources.
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Data Reduction: Image → Visibility PlaneCase Study: Imaging the halo of A2319
Subtract point source model from data, to be left with residualsand the halo. This is done in the visibility plane.
Convolve the image down to 2 arcmin, so emission from halo issmoothed out.
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Data Reduction: Image PlaneCase Study: Imaging the halo of A2319
Clean the smoothed residual+halo image. Repeat for other pointing.
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Data Reduction: Image PlaneCase Study: Imaging the halo of A2319
Mosaic the two pointings, including primary beam correction. Note: this was done in AIPS.
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Summary
Measureable of interferometers: visiblity functions (=correlatedantenna gains)
Fourier Transform visibility to get image brightness
manual calibration of visibility data necessary
science goals determine image generation
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References
Essential Radio Astronomy:www.cv.nrao.edu/course/astr534/ERA.shtml
NRAO website: nrao.edu
NRAO synthesis imaging + single dish summer schools:science.nrao.edu/opportunities/courses
VLA Observational Status Summaries:science.nrao.edu/facilities/vla/oss
CASA downloads, user manuals, etc: casa.nrao.edu/
CASA tutorials: casaguides.nrao.edu
AIPS downloads, manuals, etc: www.aips.nrao.edu/index.shtml
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