Issue |
Astron. Astrophys. Suppl. Ser.
Volume 133, Number 2, December I 1998
|
|
---|---|---|
Page(s) | 271 - 284 | |
DOI | https://doi.org/10.1051/aas:1998454 | |
Published online | 15 December 1998 |
The beam pattern of the IRAM 30–m telescope
(a reflector with several surface error distributions)
1
IRAM, 300 rue de la Piscine, Domaine Universitaire, F–38406 St. Martin d`Hères, France
2
IRAM, Nucleo Central, Avda. Divina Pastora 7, E–18012 Granada, Spain
3
I. Physikalisches Institut, Universität zu Köln, Zülpicher Straße 77, D–50937 Köln, Germany
Send offprint request to: A. Greve
Received:
28
July
1997
Accepted:
11
June
1998
Total power scans across the Moon around New Moon (mostly day time) and Full
Moon (night time) at (88 GHz), 2.0 mm (150 GHz), 1.3 mm (230
GHz), and 0.86 mm (350 GHz) wavelength are used to derive the beam pattern
of the IRAM 30–m telescope to a level of approximately
and, dependent on wavelength, to a full width of . From the reflector surface construction and application of the
antenna tolerance theory we find that the measurable beam consists of the
diffracted beam, two underlying error beams which can be explained from the
panel dimensions, and a beam deformation mostly due to large–scale
transient residual thermal deformations of the telescope structure. In view
of the multiple beam structure of the telescope, and of other
telescopes with a similar reflector construction of panels
and panel frames, we summarize the antenna tolerance theory for the
influence of several independent surface/wavefront deformations. This
theory makes use of different correlation lengths, which in essence
determine the independent error distributions, and of the
wavelength–scaling of the diffracted beam and of the error beams.
From the Moon scans we derive the parameters for calculation of the 30–m
telescope beam in the wavelength range 3 mm to 0.8 mm as required for the
reduction of astronomical observations, in particular of extended sources.
The parameters of the beam are primarily for the time after July 1997 when
the reflector was re–adjusted and improved to the illumination weighted
surface precision of σ
mm.
In the Appendix we explain the choice for this analysis of scans taken around
New Moon and Full Moon.
Key words: telescopes
© European Southern Observatory (ESO), 1998