Total Power Map to Visibilitjes (TP2VIS) Joint-Deconvolutjon of ALMA - - PowerPoint PPT Presentation

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Total Power Map to Visibilitjes (TP2VIS) Joint-Deconvolutjon of ALMA - - PowerPoint PPT Presentation

ALMA Study Total Power Map to Visibilitjes (TP2VIS) Joint-Deconvolutjon of ALMA 12m, 7m & TP Array Data Peter Teuben (U. Maryland) Jin Koda (Stony Brook/NAOJ/JAO); Tsuyoshi Sawada (NAOJ/JAO); Adele Plunketu (ESO/JAO); Crystal Brogan (NRAO)


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SLIDE 1

ALMA Study

Total Power Map to Visibilitjes (TP2VIS)

Joint-Deconvolutjon of ALMA 12m, 7m & TP Array Data

Peter Teuben (U. Maryland)

Jin Koda (Stony Brook/NAOJ/JAO); Tsuyoshi Sawada (NAOJ/JAO); Adele Plunketu (ESO/JAO); Crystal Brogan (NRAO)

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SLIDE 2

Example Science Cases with Extended & Compact Structures

  • Example science cases include

– Protostar outglows and their environment – Evolutjon of AGB stars, planetary nebulae, and their winds – Formatjon of dense clumps and pre-stellar cores in molecular clouds – Interplay between molecular clouds and galactjc structures in nearby galaxies – Galactjc outglow & fountains – Analysis of the probability distributjon functjon (PDF) from difguse, extended emission to dense, clumpy emission. – Many more

Combining data from the difgerent ALMA arrays is a science driver for a number of topics, namely those that probe size scales of extended and compact structures simultaneously.

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SLIDE 3

Example: Structure in Molecular Cloud

ALMA CO(1-0) cube of a molecular cloud in Large Magellanic Cloud

“Stomach” of molecular cloud – the entjre FoV should be fjlled with emission 12m-only 12m+7m 12m+7m+TP ALMA 12m+7m visibilitjes ALMA TP ⇒ visibilitjes (TP2VIS in MIRIAD) Demonstratjon with MIRIAD Joint-deconvolutjon (CLEAN) in MIRIAD

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SLIDE 4

Example: Structure in Molecular Cloud

ALMA CO(1-0) cube of a molecular cloud in Large Magellanic Cloud

Stomach” of molecular cloud – the entjre FoV should be fjlled with emission 12m-only 12m+7m+TP Joint-deconvolutjon: recovery of extended emission + virtually no negatjve sidelobes Demonstratjon with MIRIAD

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SLIDE 5

TP2VIS vs Feather

ALMA CO(1-0) Data of GMC in LMC; Reduced with MIRIAD TP2VIS

12m+7m+TP joint-Deconvolutjon

Feather

12m+7m Deconvolutjon + TP

Difgerence

Feather – TP2VIS

Systematjc difgerence around emission Demonstratjon with MIRIAD

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SLIDE 6

Deconvolutjon with and without TP

12m+7m+TP joint-Deconvolutjon Minus TP 12m+7m Deconvolutjon How well deconvolutjon works for 12m+7m part with and without TP? Benefjt for the 12m+7m part. Joint-deconvolutjon: Less negatjve around emission! Peaks not as good? – need more tests. Demonstratjon with MIRIAD

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SLIDE 7

ALMA Study Objectjves

  • Developments

– CASA-based TP2VIS tool – Visibility weight visualizatjon tool – Benchmark simulatjon data

  • Validatjons

– Tests with simulatjon data – Tests with ALMA archival data

  • User manuals

Our method already implemented in MIRIAD for combinatjon of CARMA and Nobeyama 45m telescope data (Koda et al. 2011). This study will make it user-friendly in CASA.

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SLIDE 8

Members and Expertjse

  • Jin Koda (Stony Brook/NAOJ/JAO)

– Developed TP2VIS in MIRIAD (Koda et al. 2011, ApJS, 193, 19) – Jump-started tests for CASA TP2VIS during his sabbatjcal at NAOJ Chile/JAO in Spring 2016; we will show some progress in this talk.

  • Peter Teuben (U. Maryland)

– One of the three founders of MIRIAD – Expertjse in CASA through the ADMIT development

  • Tsuyoshi Sawada (NAOJ/JAO)

– JAO scientjst – Expert of ALMA TP performance.

  • Adele Plunketu (ESO/JAO)

– ESO postdoc fellow at JAO – Extensive testjng of interferometer + single-dish combinatjon

  • Crystal Brogan (NRAO)

– CASA subsystem scientjst

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SLIDE 9

12m+7m+TP Combinatjon Methods

1) Initjal guess

– TP map as initjal guess for 12m+7m CLEAN

2) Feather

– Add CLEANed 12m+7m map with TP map

3) Joint-deconvolutjon (i.e., convert TP to VIS)

– CLEAN 12m+7m+TP simultaneously

Notes:

  • CLEAN could be replaced with MEM or any other deconvolutjon method
  • 3) can be used together with 1) or 2)
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SLIDE 10

TP2VIS Flow Chart

Weight Weight

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SLIDE 11

Convertjng TP map into Visibilitjes

  • Basic parameters of each visibility

– U – V – W – Amplitude – Phase – Weight

  • Supplementary parameters

– Field for mosaic – Primary beam shape – Etc.

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SLIDE 12

Convertjng TP map into Visibilitjes

  • Basic parameters of each visibility

– U – V – W – Amplitude – Phase – Weight

  • Supplementary parameters

– Field for mosaic – Primary beam shape – Etc.

Visibility distributjon set manually From Total Power (TP) map Depends on system parameters, integratjon tjmes, etc. Will try two approaches Coupled in a sense

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SLIDE 13

Gaussian Visibility/Weight Distributjon

Generate the distributjons of visibilitjes and their weights, so that their F.T. produces the TP beam patuern as synthesized beam under Natural weightjng.

htup://www.cv.nrao.edu/course/astr534/FourierTransforms.html

If the TP array has a Gaussian beam patuern, The visibility/weight distributjon should also follows a Gaussian. (U, V, W, Amplitude, Phase, Weight)

BeamTP µ e

−(l2+m

2)/2σ 2

BeamTP    

F.T. µ e −(2πσ )2(u

2+v2)/2

FWHM=2 2ln2σ

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SLIDE 14

Progress report I:

Gaussian visibility distributjon in CASA measurement set

(U, V, W, Amplitude, Phase, Weight)

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SLIDE 15

Obtain (Amp, Phase) from TP Map

(U, V, W, Amplitude, Phase, Weight)

  • Fourier-transform TP map and read (amp,phase) at a

locatjon of each visibility.

  • Learning CASAtoolkit tasks in the “simobserve” script

⇒ some success, but not fully yet.

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SLIDE 16

Weights of TP Visibilitjes

  • Among TP visibilitjes

– Two ways to adjust

  • Adjustjng visibility distributjon
  • Adjustjng weights of visibility points

⇒Already set the visibility distributjon to Gaussian. All visibility points should have an equal weight.

  • With respect to 12m+7m visibilitjes

– Best approach

  • Stjll debatable
  • Need tests

– Two approaches we plan to test

  • RMS noise-based approach
  • Matched beamsize approach

(U, V, W, Amplitude, Phase, Weight)

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SLIDE 17

Noise-based Approach: Weight from Tsys and tvis

In fact, with natural weightjng the noises of each visibility and of fjnal image are related simply: Idea: share the same proportjonality constant. (If we fjgure one out, we know the other one.) For 12m, 7m visibility For TP map (U, V, W, Amplitude, Phase, Weight) Image sensitjvity Visibility sensitjvity Calculate noise-based weight  need to the relatjon between sensitjvity and Tsys, etc. Use this for TP visibilitjes

ttot = Nvistvis

C

ij =

2kB (ηa,iA

i)(ηa,jAj)

1 2ηq

C

TP =

2kB ηm

bηaηqA

1 ∆Si      ÷

2

= 1 ∆S

k v

     ÷

2 k

∆Si µ T

sys

∆S

k

v µ T sys

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SLIDE 18

Noise-based Approach: Parameters for weights

Noise of TP single-dish map:

= RMS-noise from emission-free channels = typical Tsys from observatjons Known or measurable Arbitrarily-chosen number of visibilitjes Should be large enough to fjll UV-space smoothly (U, V, W, Amplitude, Phase, Weight)

These give the sensitjvity (or noise- based weight) of each visibility point:

∆Si = C

TP

T

sysT s ys

B× ttot

∆Si T

s ys

C

TP =

2kB ηm

bηaηqA

ttot

tvis = ttot Nvis Nvis

∆S

k v = C TP

T

sysT s ys

B× tvis

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SLIDE 19

Matched Beamsize-based Approach

CLEAN

Dirty map CLEAN components + Residual

Unit: We want to have for fmux conservatjon Depend only on weight at (u,v)=(0,0) Depend on weight distributjon in uv-space (e.g., on how extended the uv distributjon is) With TP data, the beam area and emission have non-zero values. (U, V, W, Amplitude, Phase, Weight) could cause inconsistency in fmux in a CLEANed map

Set the weight of TP data to satjsfy

Jy/Ωdirty Jy/ΩC

LEAN

Jy/Ωdirty

Ωdirty = ΩC

LEAN Ωdirty = B(l,m )dldm=W(0,0)

∫∫

Ωdirty = ΩC

LEAN

Ωdirty ≠ ΩC

LEAN

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SLIDE 20

Progress Report II

Model Smoothed with TP beam Dirty map afuer CASA/TP2VIS Difgerence

33 pointjng mosaic: x – pointjng centers We can at least make a Gaussian visibility distributjon for TP. Stjll, banging head for many issues: for example, CASA CLEAN/TCLEAN do not accept our TP visibilitjes together with 12m+7m visibilitjes … We can generate (U,V,W, Amp, Phase), but not yet other parameters

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SLIDE 21

Benchmark Model Data

  • Need model data for benchmark test for TP2VIS and
  • ther combinatjon methods in future.
  • Not so good data with emission distributjon and

dynamic range, e.g., like in molecular clouds.

  • This ALMA study will develop a set of benchmark

model data with compact & extended emission.

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SLIDE 22

Benchmark Model Data: Example

  • Power spectrum amplitude
  • Random phase
  • Test script ok, but slow (~1 week to

generate the right on a fast PC).

  • Include more coherent structure,

such as spiral arm, outglow, etc.

n=4

Resolutjon 0.05” Size 3.4’ x 3.4’

Molecular cloud with power spectrum density fmuctuatjon

P3D(k)µ k−n

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SLIDE 23

Benchmark Model Data: Example

  • Power spectrum amplitude
  • Random phase

n=4

Resolutjon 0.05” Size 3.4’ x 3.4’

Molecular cloud with power spectrum density fmuctuatjon

Shell Filament

One interestjng caveat to those who identjfy fjlaments/shells.

Even this random realizatjon shows apparent

P3D(k)µ k−n

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SLIDE 24

Documentatjon & User Manual

  • Final product include

– Descriptjon of the method – User manual

Example descriptjon

  • f the power-

spectrum model

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SLIDE 25

Summary of the New ALMA Study

Total Power Map to Visibilitjes (TP2VIS)

  • Developments

– CASA-based TP2VIS tool – Visibility weight visualizatjon tool – Benchmark simulatjon data

  • Validatjons

– Tests with simulatjon data – Tests with ALMA archival data

  • User manuals

Our method already implemented in MIRIAD for combinatjon of CARMA and Nobeyama 45m telescope data (Koda et al. 2011). This study will make it user-friendly in CASA.