Issue |
A&A
Volume 427, Number 1, November III 2004
|
|
---|---|---|
Page(s) | 377 - 386 | |
Section | Astronomical instrumentation | |
DOI | https://doi.org/10.1051/0004-6361:20035675 | |
Published online | 25 October 2004 |
Computational geometry and the design of aperture-synthesis telescopes
I. A measure of the quality of the uv-plane coverage
Institute for Astronomy, School of Physics, University of Edinburgh, Royal Observatory, Blackford Hill, Edinburgh EH9 3HJ, UK e-mail: asw@roe.ac.uk
Received:
13
November
2003
Accepted:
21
July
2004
When designing an aperture-synthesis telescope for use
in astronomy it is essential to find a layout of the antennas on
the site that provides good coverage of the uv-plane. Large
holes in the distribution of baseline points in that plane are
particularly undesirable, and so an algorithm was devised for
locating all the holes in any given design and assessing whether
they are unacceptably large. It finds, in each region of the
uv-plane, the largest circle that does not contain any of the
baseline points and then takes the properties of that empty
circle, such as the radius and the position of the centre, as
measures of the properties of the local hole. The algorithm is
based on the Delaunay triangulation of the set of baseline points
and makes use of the result that the circumscribed circle of any
Delaunay triangle is always empty. The largest empty circles in
the uv-plane are readily found in this way, and the algorithm
selects from these circles a non-overlapping set that is a good
match to the intuitive concept of the largest holes in the
distribution of baseline points. Modified algorithms are also
presented that rank each circle not by its absolute radius but by
the radius normalized to the mean radius of the circles in the
same neighbourhood of the uv-plane; these versions make proper
allowance for the large-scale variation of the density of
baselines caused by the taper and are therefore of greater use to
the designers of a telescope. The algorithms are efficient,
requiring O
operations where NB is the number of baselines, and may
be used in several ways. One is to take the radius of the largest
empty circle as a figure of demerit so that, of a set of trial
configurations, the one with the smallest value may be regarded as
having the best uv-plane coverage. Another is to take the
baselines on the circumference of the largest circle to indicate
which antennas are the most suitable for repositioning in order to
improve the quality of the uv-plane coverage of a trial
configuration.
Key words: telescopes / instrumentation: interferometers
© ESO, 2004
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