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van Cittert-Zernike Theorem Fundamentals of Radio Interferometry, Section 4.5 Griffin Foster SKA SA/Rhodes University NASSP 2016

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  • van Cittert-Zernike TheoremFundamentals of Radio Interferometry, Section 4.5

    Griffin FosterSKA SA/Rhodes University

    NASSP 2016

  • NASSP 2016 2:21

    What is the Fourier transform of the sky?

  • NASSP 2016 3:21

    Important Points:

    The van Cittert-Zernike Theorem is at the heart of aperture synthesis.

    Fourier transforms are essential to synthesis imaging.

  • NASSP 2016 4:21

    Simply stated: there exists a relationship between the mutual spatial coherence function and the sky intensity distribution. This relationship can be approximated as:

    The mutual spatial coherence function (visibilities) and the sky intensity distribution (image of the sky) are Fourier pairs

    van Cittert-Zernike Theorem

  • NASSP 2016 5:21

    Mutual Spatial Coherence Function

    Given a signal, in our case the electric field (E), the mutual spatial coherence function for two point in space

    (r1, r2) is the time-averaged correlation of the signal

    measured at each point.

    The mutual spatial coherence function is a correlation between two points in space, in our case, two radio antennas.

  • NASSP 2016 6:21

    Mutual Spatial Coherence Function

    In aperture synthesis we call the mutual spatial coherence function the Visibility function. Instead of the

    absolute position of each point we instead use the spatial difference

    Thus, the Visibility function is in the uvw-space.

  • NASSP 2016 7:21

    Sky Intensity Distribution

    The sky intensity distribution is a fancy name for what the sky looks like at a given frequency ν. For the van

    Cittert-Zernike theorem we use the direction-cosine reference frame.

  • NASSP 2016 8:21

  • NASSP 2016 9:21

    Hand-wavy Derivation

    Image of the Sky

  • NASSP 2016 10:21

    Hand-wavy Derivation

    1. Given a source far away, such as an astronomical object, the electric field from that source can be considered a plane wave (i.e. the source is in the far-field).

  • NASSP 2016 11:21

    Hand-wavy Derivation

    2. We measure the electric field at two spatially separated points r1, r2.

  • NASSP 2016 12:21

    Hand-wavy Derivation

    3. For any two point in space in which we measure the electric field there is a phase difference between the measured signals which results in a constructive or destructive interference depending on the relative position of the two measurement points and the observing frequency.

  • NASSP 2016 13:21

    Hand-wavy Derivation

    4. For any relative spatial difference there is this phase difference is constant.

    Geometric Delay:

    Phase:

  • NASSP 2016 14:21

    Hand-wavy Derivation

    5. This fringe pattern results in a sinusoidal wave in the 2-D mutual spatial coherence space.

    Fringe PatternGeometric Delay:

    Phase:

  • NASSP 2016 15:21

    Hand-wavy Derivation

    6. The Fourier transform of a sinusoidal function is a delta function at a particular position, i.e. the source of the electric field in the sky.

    Visibility Function Image of the Sky

  • NASSP 2016 16:21

    Real Derivation

    See Interferometry and Synthesis in Radio Astronomy (TMS) Chapter 14

  • NASSP 2016 17:21

    The more complete van Cittert-Zernike Theorem

    Our 2-D Fourier relation between the visibility function and the sky is an approximate form of the van Cittert-Zernike theorem:

    A more complete version of van Cittert-Zernike is:

    Unfortunately, this is not a 2-D Fourier relation.

  • NASSP 2016 18:21

    Approximations to reduce to a 2D Fourier transform

    Small Angle/Narrow Field of View Approximation:

    If we are only interested in a small area on the sky then the extant of (l,m) is small:

    From positional astronomy, the sky instensity is distributed on the celestial (unit) sphere such that for any position (l,m,n):

    Then the van Cittert-Zernike theorem can be approximated as:

  • NASSP 2016 19:21

    Approximations to reduce to a 2D Fourier transform

    Delay term/w-term Approximation:

    If our visibility sampling is approximately on a plane, or again we are only interested in a narrow field of view

    then the so-called w-term

    can be seen as a constant delay term, with a simple correction w=0.

  • NASSP 2016 20:21

    What is the Fourier transform of the sky?

  • NASSP 2016 21:21

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