SKA Working Group 1: Milky Way and Nearby Galaxies

Compliance Matrix for Level 0 Science Goals



Level 0 Science Goal
Canada
China 
Europe 
India 
Ozlens 
Ozcyli 
USA 
HI in the Universe   notes
3 notes
2 notes
4 notes
5 notes
5 notes
5 notes
4 notes
Magnetic Universe   notes
3 notes
2 notes
1 notes
4 notes
3 notes
4 notes
3 notes

Numerical scale calibration :
5 = complete compliance

3 = compliance could be reached with significant (but not fundamental) changes to the proposed design
1= no possible compliance

Links to earlier versions:  The SKA Concept    SKA designs-requirements matrix: HI  Preliminary all-WG compliance matrix





HI in the Universe

HI (neutral atomic hydrogen) is the fundamental tracer of neutral gas in the universe at all times and on all scales. The SKA will provide an unprecedented view of the structure and motion of gas inside and outside of galaxy disks. The SKA will be able to survey HI 21-cm emission from large numbers of spiral and dwarf irregular galaxies (out to z~1), and to map the distribution of the HI  in the Milky Way at unprecedented resolution and sensitivity.  This encompasses level-1 science for working groups 1, 3 and 4.


General comments on design compliance for HI science :


A hypothetical mapping project would need brightness temperature sensitivity 1 K over spectral channel width 5 kHz with beam size 10 arc seconds.  We should be able to survey at a rate of 1 square degree per hour or faster with this combination of sensitivity and resolution.  At 21-cm wavelength this requires a large fraction of the collecting area (~50%) at baselines shorter than 5 km.  

* Frequency range: 1.4 GHz only

* Multibeaming: not needed provided the field of view requirement is met.

* Array configuration: continuous u-v coverage needed giving angular resolution over the full range from 1 arcsec to 30 arcmin at 1.4 GHz (20m to 40 km baselines).

* Field-of-view: minimum of 1 square degree for core of array at 1.4 GHz with full brightness sensitivity.  A significant fraction of 1
square degree must be able to be imaged for baselines out to 50 km

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HI specific notes:


 Chinese design for HI

COMPLIANCE RATING: 2

COMMENTS:

* The field of view is insufficient for imaging local galaxies,
or for surveying regions of the Milky Way.

* This science goal requires continuous u-v coverage giving resolution from 1 arc second to ~30 arcmin. The gap in spacings between 200-1000 metres, is a major problem for mapping HI, which contains power on all spatial scales.

* It would be extremely beneficial to be able to do 21cm spectral line and continuum simultaneously

* Spacings shorter than 200m seem only to be available by making single-dish measurements and then combining them with the interferometer data at the reduction stage. This will limit dynamic range when imaging large faint structure.

* The main specification of HI surveys is to reach a brightness sensitivity of 1K in survey mode (approx 1 deg^2/hr) at a resolution substantially better than 1 arcmin. It will be challenging to achieve these goals with this design to achieve a brightness sensitivity of 1K with any subset of the array because of the lack of close packing.

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European design for HI

COMPLIANCE RATING: 4

COMMENTS:

* What is the u-v coverage within the core? If only individual stations correlated, sensitivity to large spatial scales will be limited.

* While the brightness sensitivity in this design is limited by small collecting area of core, multibeaming makes up for this, letting one
survey several areas at once.

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Indian design for HI

COMPLIANCE RATING: 5

COMMENTS:

* While available specifications for this design meet our requirements, more information is needed on array configurations etc.

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USA design for HI

COMPLIANCE RATING: 4

COMMENTS:

* While the brightness sensitivity of this design is limited at intermediate resolutions, the very dense core ensures that efficient HI
surveying can still be done. 

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Canadian design for HI

COMPLIANCE RATING: 3

COMMENTS:

* This science goal requires continuous sensitivity at resolutions from 1arc second to ~30 arcmin. The gap in spacings between 200-1000 metres is a major problem for mapping HI, which contains power on all spatial scales.

* It would be extremely beneficial to be able to do 21cm spectral line and continuum simultaneously

* Spacings shorter than 200m seem only to be available by making single-dish measurements and then combining them with the interferometer data at the reduction stage. This will limit dynamic range when imaging large faint structure.

* The main specification of HI surveys is to reach a brightness sensitivity of 1K in survey mode (approx 1 deg^2/hr) at a resolution
substantially better than 1 arcmin. It will be challenging to achieve these goals with this design to achieve a brightness sensitivity of 1K
with any subset of the array because of the lack of close packing.

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  Australian Cylinder  design for HI
No problems noted.

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 Australian Luneberg Lens  design for HI
No problems noted.
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The Magnetic Universe

Magnetic fields are fundamental to most physical processes in the Universe, but are usually overlooked. The techniques and processes with which one can easily map the strength and structure of magnetic fields are unique to radio astronomy. The SKA will be able to map the strength and direction of the magnetic fields in the Milky Way and nearby galaxies in several ways. These include Zeeman splitting of the 21-cm and OH maser lines, measurement of the linear polarization of synchrotron emission (both in discrete sources and the diffuse Galactic background), and measurement of the Faraday rotation of linear polarization toward pulsars, extragalactic sources, and the diffuse synchrotron emission.  Some of these applications require very high brightness sensitivity, including good sensitivity to very short uv spacings.  This topic encompasses level-1 science goals for working groups 1, 2, 6 and 8.

General comments on design compliance:

A hypothetical polarization mapping project would need brightness temperature sensitivity 0.01 K over  bandwidth 5 MHz with beam size 10 arc seconds.  We should be able to survey Stokes Q,  U, and V at a rate of 1 square degree per hour or faster with this combination of sensitivity and resolution.  This requires about half the total collecting area be in a central core with diameter ~ 5 km.   

* Frequency range: 0.4-8 GHz  (0.4-12 GHz desirable)

* Multibeaming: not needed

* Array configuration: continuous u-v coverage needed over scales
giving angular resolution over the full range of angular resolution  ~0.5 arcsec to 30 arcmin at 1.4 GHz (20m to 40 km baselines).

* Field-of-view: 1 square degree at 1.4 GHz; need to be able to image full FOV out to baselines of 100 km.

* Other: Polarization purity of -40 dB needs to be attainable over the entire field of view. -30 dB should be attainable in hardware, with a further 10 dB after calibration.


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Polarization specific notes:




Chinese design for Galactic magnetic fields & polarization

COMPLIANCE RATING: 2

COMMENTS:

* The field of view is insufficient for imaging local galaxies, or for surveying regions of the Milky Way.

* This science goal requires continuous sensitivity with resolution from 0.5" to ~30' for mapping diffuse emission in other galaxies, as well as for studying individual objects in our own Galaxy. Also, the relatively small number of elements (30) might limit the continuity of the u-v coverage at
longer spacings.

* Spacings shorter than 200m seem to only be available by making single-dish measurements and then combining them with the interferometer data at the reduction stage. Calibration will need to be extremely accurate for polarimetry studies; also, this will limit dynamic range when imaging large faint structure.

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Indian design for Galactic magnetic fields & polarization

COMPLIANCE RATING: 4

COMMENTS:

* Can a 1 deg^2 FOV be achieved at 0.5 arcsec resolution (at 1.4 GHz)? Or will the antenna elements be grouped into stations?

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European design for Galactic magnetic fields & polarization

COMPLIANCE RATING: 1

COMMENTS:

* The limited frequency coverage of this design will make it very difficult to study polarization, because of heavy depolarization at
lower frequencies.

* This science goal requires continuous sensitivity with angular resolution from 0.5" to ~30'. It needs to be determined whether the 70 non-VLBI stations in this design can provide sufficient u-v coverage and dynamic range to meet this goal.

* Can a 1 deg^2 FOV be achieved at 0.5 arcsec resolution (at 1.4 GHz)? Or does the station concept limit the FOV?

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Australian lens design for Galactic magnetic fields & polarization

COMPLIANCE RATING: 3

COMMENTS:

* The limited frequency coverage of this design will make it difficult to study polarization, because of depolarization at frequencies below
~8-10 GHz.

* The station size of 250 metres limits the FOV at subarcsec resolution to << 1 deg^2

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  Australian cylinder design for Galactic magnetic fields & polarization

COMPLIANCE RATING: 4

COMMENTS:

* The offset line feed design (preferred) may have difficulty providing the required polarization performance.  Asymetrical beam patterns in Stokes Q and U may be unavoidable.

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USA design for Galactic magnetic fields & polarization

COMPLIANCE RATING: 3

COMMENTS:

* The station size of 84 metres limits the FOV at subarcsec resolution to << 1 deg^2

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Canadian design for Galactic magnetic fields & polarization

COMPLIANCE RATING: 3

COMMENTS:

* This science goal requires continuous sensitivity with angular resolution from 0.5" to ~30' for mapping diffuse emission in other galaxies, as well as for studying individual objects in our own Galaxy. Also, the relatively small number of elements (60) might limit the continuity of the u-v coverage at longer spacings.

* Spacings shorter than 200m seem to only be available by making single-dish measurements and then combining them with the interferometer data at the reduction stage. Calibration will need to be extremely accurate for polarimetry studies; also, this will limit dynamic range when imaging large faint structure.

* Polarimetry studies can greatly benefit from simultaneous observations in two separate frequency bands, for Faraday rotation
studies. With only one independent IF, one can do these observations in serial fashion, but at lower efficiency.

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