B3 - Note for Users
|
Receiver B3 (345GHz band) Current Status:
Notes for Users
|
(TSS notes here)
Introduction
B3 is the JCMT facility instrument for spectral line observations in
the 345-GHz (0.8mm) band. It consists of two independent SIS mixers
which detect orthogonally-polarised radiation at the same
frequency. One can choose to observe with either one mixer, or both in
parallel.
Recent changes
In January 2000 the second of the two mixers was replaced with a
tunerless version. Both mixers cover a similar frequency range with
similar noise characteristics, although at the higher frequencies, at
360 GHz and above, the new mixer has a fairly sharp upturn in noise
temperature
For those with some familiarity with B3, here are some additional
details:
- With the installation of the second mixer in channel A another
moving part, the mixer backshort, was removed. The backshort drive
mechanisms are still both in place, but without connection to the
mixer block, and are set to a fixed value for all frequencies. The
control software calling for tuning of the backshort positions has
been disabled. Leaving the external backshort drives in place allows
the spare tuned mixer to replace a mixer should one fail, since there
is presently no spare.
- In mid-1999 the mixer in channel B was replaced with the new
tunerless version, and the tuned mixer in channel A swapped for the
one originally in channel B. The mixer block taken from channel A was
sent back to HIA where it was been converted to a tunerless
version. The original channel A had developed a nasty fault: an
increase in noise by about 50% about 100 MHz wide in the center of the
IF band. A postmortem on the mixer (see
picture provided by Charles Cunningham) shows that the entire
structure had been shifted off-center under pressure from the contact
bellows.
- B3 has had a record of operational problems, which had
considerably worsened in the early part of 1999. The main focus of the
work during B3's protracted absence from the cabin in mid-1999 was an
overhaul of the fairly complex control electronics, mechanical
components and related software. This work took much longer than
expected, and some revisions of the on-board microcomputer code were
necessary.
Performance expectations for B3
Only a limited number of observations have been made since the most
recent changes, but the results are very good. The pointing and focus
offsets were within normal expectations, and the alignment of the two
beams differs by about 1 arcsec. A quick observation of Mars under
daytime conditions immediately after installation on 18 January 2000
gave a beam efficiency of about 0.63 for channel B, close to
nominal. Channel A was about 5% lower, perhaps because of the relative
beam alignment. Observations of the standard line sources gave line
strengths which were well within normal variations from night to night
and very close to equal in strength.
No dedicated commissioning tests have been carried out so far, and
although it appears that users can expect the modified B3 to behave
almost identically to the previous versions of the receiver, all
observers would be well advised to obtain, at the least, spectra toward
standard sources for comparison with existing data. It would be useful
also to make observations especially of the planets Mars and Uranus if
possible in order to obtain antenna and beam efficiencies. Beam maps
would be really nice to have, but need to be obtained only under
stable and dry conditions to be useful.
B3 has been found to tune reasonably reliably between LO frequencies
of 322 and 369 GHz; that is, sky frequencies from 318 to 373 GHz
should be accessible with both mixers. In the absence of any faults B3
now tunes from one frequency to another within about 15 seconds. Some
operational idiosyncracies still exist, but in general there are
workarounds known to the telescope operators for those oddities that
remain. Double-sideband receiver temperatures are about 110-120K for both
mixers across the band with the exception of the upper reaches of
channel A. We will provide plots showing the final numbers once we
have had the opportunity to carry out this work.
Both channels of B3 are capable of observing a window 920 MHz
wide. Channel B should be used for wideband work up to the
spectrometer maximum of 1.8 GHz instantaneous bandwidth, since the
band is somewhat limited by the HEMT amplifier in channel A.
The future
We will be continuing improvements to the operation of B3, involving
all aspects of control. We expect to make further changes to the
microcomputer code and in in due course remove various elements of the
system which are no longer necessary now that both mixers have fixed
backshorts.
|