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UKIRT Observing Conditions
| CONDITION REQUIREMENTS FOR
UKIRT OBSERVING |
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UKIRT is flexibly scheduled, and it is important that PIs specify
their requirements in terms of seeing, water vapour and sky brightness adequately
for their observing programmes to be feasible. This document lists the effects
of weather on various types of observing.
Seeing
This is a function of the science and PIs should simply specify what
they require. However, some guidance as to the seeing behaviour may be useful:
(i) seeing currently improves markedly (by, say 0.3 arcseconds) during
the first hour of the night, and thereafter decreases very slowly (by another
0.1 arcsecond) into the small hours of the morning. This variation is statistical
in nature only, and cannot be relied upon to happen on any given night.
(ii) seeing is better in the summer and early autumn than it is through
the winter months. This is again a statistical statement - the difference
is small (of order 0.1 arcseconds on a median around 0.5 in the K band)
and it is probably also a function of the Pacific ocean circulations - el
Nino years (on a sample of one) may be better than others. The median seeing
at UKIRT varied from 0.45 in the el-Nino year of 1998, to 0.55 arcseconds
in 1999.
Water vapour
It is hard to place a hard and fast limit on the properties of water
vapour absorptions on observed data, because the water lines are highly
wavelength-dependent and variable. The UKIRT observing tool will initially
allow observers to specify whether they require "dry" conditions, which at
the telescope will be defined by a single tau cutoff of 0.09. This should
be requested by PIs on programmes involving:
(i) spectroscopy and imaging in the three-micron window, particularly
spectroscopy around 3.2 microns. Programmes concentrating on the long end
of the window may be possible in worse conditions;
(ii) programmes of spectroscopy on the fringes of the 10-micron window
and anywhere in the 20-micron band;
(iii) photometric programmes in the broad N filter and narrow filters
in the Q band.
(iv) spectroscopy requiring contiguous coverage
of the entire JHK window.
Further details of the statistical behaviour of the water vapour content
above MKO are given here.
Sky Brightness
Sky brightness in the near-infrared is dominated by photochemically-driven
variations in the atmospheric OH emission. This is principally seen in
the J and H bands, where the variation is pronounced and continual from
sunset through to dawn. The J-band sky brightness shows the greatest variations,
with a magnitude drop in the first hour after sunset and a further magnitude
drop distributed through the rest of the night; a similar but slightly
less dramatic decrease is seen in the H and K bands. Figures posted here show
these variations in mag/sq arcsecond at zenith measured throughout an observing
year. They are intended as a guide only, no attempt has been made to filter
for poor weather or proximity to the moon (in practice it is time of the
night which produces the greatest variations). In the thermal-IR (three
microns and longer) the sky brightness is constant (and very high) and
there is no particular preferred time of night.
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