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)
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)
Jin Koda (Stony Brook/NAOJ/JAO); Tsuyoshi Sawada (NAOJ/JAO); Adele Plunketu (ESO/JAO); Crystal Brogan (NRAO)
– 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.
“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
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
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
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
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.
– 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.
– One of the three founders of MIRIAD – Expertjse in CASA through the ADMIT development
– JAO scientjst – Expert of ALMA TP performance.
– ESO postdoc fellow at JAO – Extensive testjng of interferometer + single-dish combinatjon
– CASA subsystem scientjst
Notes:
Weight Weight
Visibility distributjon set manually From Total Power (TP) map Depends on system parameters, integratjon tjmes, etc. Will try two approaches Coupled in a sense
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
(U, V, W, Amplitude, Phase, Weight)
(U, V, W, Amplitude, Phase, Weight)
– Two ways to adjust
⇒Already set the visibility distributjon to Gaussian. All visibility points should have an equal weight.
– Best approach
– Two approaches we plan to test
(U, V, W, Amplitude, Phase, Weight)
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
sys
k
v µ T sys
= 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)
∆Si = C
TP
T
sysT s ys
B× ttot
s ys
C
TP =
2kB ηm
bηaηqA
∆S
k v = C TP
T
sysT s ys
B× tvis
CLEAN
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
LEAN
LEAN Ωdirty = B(l,m )dldm=W(0,0)
LEAN
Ωdirty ≠ ΩC
LEAN
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
generate the right on a fast PC).
such as spiral arm, outglow, etc.
n=4
Resolutjon 0.05” Size 3.4’ x 3.4’
Molecular cloud with power spectrum density fmuctuatjon
n=4
Resolutjon 0.05” Size 3.4’ x 3.4’
Molecular cloud with power spectrum density fmuctuatjon
One interestjng caveat to those who identjfy fjlaments/shells.
Even this random realizatjon shows apparent
Example descriptjon
spectrum model
Total Power Map to Visibilitjes (TP2VIS)
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.