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Radio Interferometry and ALMA T. L. Wilson ESO

Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

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Page 1: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Radio Interferometry and ALMA

T. L. Wilson

ESO

Page 2: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

A few basics:

Wavelength and frequency -1

temperature max(mm) ~ 3/T(K)(for blackbody)

Hot gas radiates in X rays or optical, cooler gas in FIR. mm

Angles: resolution of ALMA=0.2 (mm)/baseline(km)(at =1 mm, ALMA better than HST)

Flux Density and Temperature in the Rayleigh-Jeans limit: S(mJy)=73.6 T(K) (’’)/ (mm)

Minimum theoretical receiver noise: Trx=h/k=5.5( /115 GHz)

Sensitivity calculator: ESO home page under ALMA

Page 3: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Opacity of the Atmosphere

Page 4: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Prime focus

Secondary focus

A parabolic radio telescope

Page 5: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Cover up parts of the dish.Thensample only certain structuralcomponentsof the source

Page 6: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

The regionswherepower is receivedare widerapart, so oneis sensitiveto smaller structures

Page 7: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Sketch of 2 element interferometer

Page 8: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Equations to describe 2 element interferometer

Page 9: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Dirty Beams, Improving Images

Page 10: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

A single source, not centered by the interferometer

Page 11: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

A double sourcewith equal intensity

Page 12: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

(u,v) plane and image plane

• These are related by Fourier transforms

• The previous relationships are valid, but are cast in a different form

• On the next overhead, we show some plots of the amplitude and phase of u for one dimensional distributions

Page 13: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

1-Dimensional distributions in the u and image planes

u planedistribution in amplitudeand phase

Imageplane distributions for simple sources

Page 14: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Earth Rotation Aperture Synthesis

Above: the 2antennas onthe earth’s surface have a different orientation as a function of time.

Below: the ordering of correlated data in (u,v) plane.

Page 15: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Gridding and sampling in (u,v) plane

Page 16: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

VLA picture

Inner part of the compact configuration of the Very Large Array

Page 17: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

VLA uv plane response

Page 18: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Dataas taken

Datawith MEM

Data with MEMand Self-Calibration

The radiogalaxy Cygnus Aas measured with all configurations of the VLA

Page 19: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

A Next Generation Millimeter Telescope

A major step in astronomy a mm/submm equivalent of VLT, HST, NGST, EVLA

• Capable of seeing star-forming galaxies across the Universe• Capable of seeing star-forming regions across the Galaxy

These Objectives Require:• An angular resolution of 0.1” at 3 mm• A collecting area of >7,000 sq m• An array of antennas• A site which is high, dry, large, flat - a high Andean plateau is

ideal

Page 20: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

• A mm/submm equivalent of VLT, NGST

• 64 x 12-meter antennas, surface < 25 µm rms

• Zoom array: 150m 16 kilometers

• Receivers covering wavelengths 0.3 - 10 mm

• Located at Chajnantor (Chile), altitude 5000 m

• Europe and North America sharing the construction (US$552 million) cost and operations costs

• Hopefully Japan will soon join!

http://www.eso.org/projects/alma/

ALMA: The Atacama Large Millimeter Array

Page 21: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

10 km

The ALMA site: Chajnantor, Chile Altitude 5000m

ALMA Site

Page 22: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

ALMA Compact Configuration

Page 23: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

ALMA Intermediate Configuration

Page 24: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

ALMA extended configuration

Page 25: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

Simulations: L. Mundy

Page 26: Radio Interferometry and ALMA T. L. Wilson ESO. A few basics: Wavelength and frequency  -1 temperature max (mm) ~ 3/T(K) (for blackbody) Hot gas radiates

The Atacama Large Millimeter Array

ALMA