Radio interferometry
Pierre Hily-Blant
Université Grenoble Alpes 2020-21 (All lectures here)
Orders of magnitude
How to increase the sensitivity of a single-dish ?
ALMA interferometer
Protoplanetary disks observed with ALMA
IRAM/NOEMA interferometer
ESO/VLT Interferometer
Applications of interferometry
Applications of interferometry
Optical vs Radio interferometry
Warning
Twin-element interferometer
The Michelson-Pease interferometer: measuring stellar diameters
Extended source seen with the twin-elements interferometer
The first radio interferometer
February 7th 1946, Dover Heights, Sydney, McCready, Pawsey, and Payne-Scott 1947
Early additive interferometer
Recall the general relationships between the various functions:
Fourier space view
Visibility of the additive interferometer
Problems with the additive interferometer
Phase-switched interferometer
Fourier analysis
Advantages of the multiplying interferometer
Multi-antenna interferometer
Synthesis imaging
Low-pass vs Pass-band filters
Zero-spacings
Cygnus A: from early to modern interferometers
Figure 35: Synthesis image of Cygnus A (AGN) using Earth rotation with the Cambridge One-Mile Radio Telescope; 1.4 GHz (Ryle+65)
Figure 36: Cygnus A with the Cambridge Five-Kilometre Radio Telescope; 5 GHz (Ryle+65)
Figure 37: Synthesis image with four configurations of the VLA at 4.9 GHz; 0.4" resolution (Perley+84)
Figure 38: VLBI image 5 GHz; 0.002" resolution (Carilli+94)
Correlator output from dΩ, within dν:
\(dr = \frac{1}{2} A(\vec{\sigma})I(\vec{\sigma})\cos(\omega\tau_g)d\Omega d\nu\)
Extended source
Correlator output from all (incoherent) source elements:
\[r = 1/2 d\nu\int_{4\pi} A(\vec{\sigma})I(\vec{\sigma})\cos(2\pi \vec{b}\cdot\vec{s}/\lambda)d\Omega\]
We define the complex visibility by:
\[ {\cal V} = |{\cal V}|e^{i\Phi_{\cal V}} = \frac{1}{P(0)} \int_{4\pi} A(\vec{\sigma})I(\vec{\sigma}) e^{-i 2\pi\nu_0 \vec{b}\cdot\vec{\sigma}}d\Omega \]
Correlator output can then be written:
2r(t)/dν = cos(2πτg ν0) Re(V) + sin(2πτg ν0) Im(V) = |V| cos[2πν0 τ0(t) - ΦV]
Bandwidth pattern
Receivers have a finite bandwidth (ν=ν0 ± Δν/2): the fringe pattern cos(ωτ) is multiplied by the 'envelope' (FT of H-function is a sinc)
FB(θ)=sin(πΔντg)/(πΔντg), τg=b sinθ/c≈ bθ/c
Instrumental delay τI and phase reference center
Visibility:
\(V(u,v,w) = \frac{1}{\sqrt{1-x^2-y^2}} \int\int A(x,y)I(x,y)e^{-i2\pi(ux+vy)}e^{-i\pi(x^2+y^2)w}dxdy\)
What are visibilities?
If the field of view is small enough, \(\pi(x^2+y^2)w\) can be neglected, this reduces to a 2D Fourier transform:
\(V(u,v) \approx V(u,v,0) = \int_{-\infty}^\infty\int_{-\infty}^\infty \frac{A(x,y)I(x,y)}{\sqrt{1-x^2-y^2}}e^{-i2\pi(ux+vy)}dxdy\)
Image synthesis
Dirty beam: 2 antenna
taken from Lecture by D. Wilner
Note the reversed x-axis in the direct (dirty beam) plane
Image Synthesis: increasing the number of antenna
Adapted from Lecture by D. Wilner
Super Synthesis: increasing the number of samples (Earth rotation)
Adapted from Lecture by D. Wilner
Field of view and zero-spacings
Summary
Created by PHB