Slide 1
A Crash Course in Radio Astronomy and Interferometry: 1. Basic Radio/mm Astronomy
James Di Francesco
National Research Council of Canada
North American ALMA Regional Center – Victoria
(thanks to S. Dougherty, C. Chandler, D. Wilner & C. Brogan)
Slide 2
EM power in bandwidth dn from solid angle dW intercepted by surface dA is:
Defines surface brightness Iv (W m-2 Hz-1 sr-1 ; aka specific intensity)
Flux density Sv (W m-2 Hz-1) – integrate brightness over solid angle of source
Convenient unit – the Jansky 1 Jy = 10-26 W m-2 Hz-1 = 10-23 erg s-1 cm-2 Hz-1
Basic Radio/mm Astronomy
Slide 3
In general surface brightness is position dependent, ie. In = In(q,f)
(if In described by a blackbody in the Rayleigh-Jeans limit; hn/kT << 1)
Back to flux:
In general, a radio telescope maps the temperature distribution of the sky
Basic Radio/mm Astronomy
Slide 4
Many astronomical sources DO NOT emit as blackbodies!
However….
Brightness temperature (TB) of a source is defined as the temperature of a blackbody with the same surface brightness at a given frequency:
This implies that the flux density
Brightness Temperature
Slide 5
Recall :
Telescope of effective area Ae receives power Prec per unit frequency from an unpolarized source but is only sensitive to one mode of polarization:
Telescope is sensitive to radiation from more than one direction with relative sensitivity given by the normalized antenna pattern PN(q,j):
Basic Radio Astronomy
Slide 6
Johnson-Nyquist theorem (1928):
Antenna temperature is what is observed by the radio telescope.
Power received by the antenna:
A “convolution” of sky brightness with the beam pattern
It is an inversion problem to determine the source temperature distribution.
Basic Radio Astronomy
Slide 7
The antenna collects the E-field over the aperture at the focus
The feed horn at the focus adds the fields together, guides signal to the front end
Basic Radio/mm Astronomy
Slide 8