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% 1 The UKIRT Infrared Deep Sky Survey (UKIDSS)UKIDSS
%     1.1  Introduction  
%     1.2  Achievements of UKIDSS   
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% 2 The Galactic Plane Survey (GPS)
%     2.1  Introduction : original science case
%     2.2  Progress on the GPS survey 
%     2.3  Case for completion of GPS
%     2.4  Comparison with other surveys     
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% 3  Technical case
%     3.1 UKIDSS implementation 
%     3.2 Completion of GPS 
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% 4  Data Management 
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% 5  Collaborators and Institutions
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% 6 References     
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\title{\vspace*{-3cm}
Proposal to UKIRT Board \\
Completion of UKIDSS Galactic Clusters Survey (GCS)}

\author{N.Hambly \\
University of Edinburgh, \\
Head of UKIDSS GCS Working Group}

\date{Nov 3 2006}

\pagestyle{myheadings}
\markboth
{UKIDSS GCS completion}
{UKIDSS GCS completion}
\thispagestyle{empty}


\begin{document}

\maketitle

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%                ABSTRACT        
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\begin{abstract}
The UKIDSS Galactic Clusters Survey aims to measure the substellar 
mass function (MF) in ten young Galactic open clusters and 
star formation associations. We intend to
determine, with good statistics, the form of this function down to 
between 10 and 40 Jupiter masses (depending on cluster age/distance) 
in a variety
of Galactic environments. These observations will yield an accurate and uniform
census of the present day MF as a function of local Galactic environment and
age. Furthermore, the GCS will enable determination of the underlying
initial MF in those environments, and will provide observational data to
critically confront the latest models of the fundamental astrophysical 
formation process for substellar objects.
\end{abstract}


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%               GENERAL UKIDSS DESCRIPTION
%  UKIRT guidance for overall science case : <= 8 pages including figures
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\section{The UKIRT Infrared Deep Sky Survey (UKIDSS)}  \label{UKIDSS}

\subsection{Introduction}

The UKIRT Infrared Deep Sky Survey (UKIDSS) is the most significant step forward
in infrared sky surveys since the Two Micron All Sky Survey Project (2MASS; Skrutskie \et\ 2006),
and can be considered
the near-infrared counterpart of the Sloan Digital Sky Survey (SDSS; York \et\ 2000). It
does not
cover the whole sky, but is many times deeper than 2MASS. It is in fact
not a single survey but a survey programme combining a set of five
survey components of complementary combinations of depth and
area. The Large Area Survey, the Galactic Cluster Survey, and the Galactic Plane Survey cover approximately 7000 square degrees to a depth of K$\sim$18; the Deep Extragalactic Survey covers 35 square degrees to K$\sim$21, and the Ultra Deep Survey covers 0.77 square degrees to K$\sim$23. 
The prime aim of UKIDSS is to provide a long term astronomical legacy database; the design is however driven by a series of specific goals -- for example to find the nearest and faintest sub-stellar objects; to break the z=7 quasar barrier; to determine the epoch of re-ionisation; to determine the substellar mass function; to discover Population II brown dwarfs, if they exist; to measure the growth of structure from z=3 to the present day; to determine the epoch of spheroid formation; and to map the Milky Way through the dust, to several kpc. The survey data are being uniformly processed and made available in a series of well documented staged releases. The data are immediately public to astronomers in all ESO member states, and available to the world after eighteen months. 

UKIDSS was proposed to the UKIRT Board in March 2001 as a seven year programme, using approximately one thousand nights of time with the UKIRT Wide Field Camera (WFCAM). The full programme was provisionally
approved, with an initial two-year programme followed by an expected review of progress to confirm the full seven year programme. The UKIDSS progress review is being provided separately, while the proposal to complete the full programme is being considered as part of the UKIRT Survey Call. Following Board guidance, a separate completion proposal is being made for each of the component surveys within the UKIDSS programme (LAS, GPS, GCS, DXS, UDS). However, it is important to understand that UKIDSS is designed, planned, and implemented as a single interacting whole. UKIDSS is fully described in Lawrence \et\ (2006; astro-ph/0604426). 
The original science case is available on the
UKIDSS project web pages at http://www.ukidss.org. 

\subsection{Achievements of UKIDSS}

After many years of planning, UKIDSS is now a successful reality, thanks to close collaboration between UKIRT, VDFS, and the members of the UKIDSS consortium, who have designed and implemented observing strategy, organised the registration of archive users across Europe, and in collaboration with the VDFS team, carried out quality control filtering, produced stacked and merged survey products, and achieved two public data releases : the Early Data Release (EDR, January 2006), and the First Data Release (DR1, July 2006). The DR1 release contains 7\% of the likely final volume of UKIDSS, and is already bigger than 2MASS. The coverage to date is shown in Table 1. Four technical papers describing the survey, photometric system, and data release details have been published or are in press (Lawrence \et\ 2006, Hewett \et\ 2006, Dye \et\ 2006, Warren \et\ 2006) and four more papers are in preparation describing the camera, the pipeline, the archive, and the survey calibration (Casali \et , Irwin \et , Hambly \et , Hodgkin \et ).

These data releases attracted considerable attention, in the media and amongst professional astronomers. Use of the data has been very impressive. Since EDR release there have been over 7000 queries from 40 different institutions exporting over one billion rows. Papers are already appearing. We are currently aware of 20 UKIDSS related papers either in press, on astro-ph, or in preparation. The ones we know about are from members of UKIDSS working groups, and so we imagine there are many more in preparation across Europe. These papers are based on the tiny volume of data in the EDR; many more will follow using DR1. These early papers, and unpublished work we are aware of, include some impressive results - a quasar at $z=5.86$; discovery of one of the coolest known T-dwarfs; discovery of 9 luminous Lyman-break galaxies at $z>5$; determination of the K-band luminosity function and its evolution to unprecedented accuracy in the range $0.5<z<2$; and location of dozens of brown dwarfs down to 30 Jupiter masses in two clusters. 

\begin{table}
\centering
\begin{tabular}{@{}lrcc@{}}
\hline
\multicolumn{1}{c}{Survey} &\multicolumn{1}{c}{Area} & Filters & K
5$\sigma$ depth \\ 
     & \multicolumn{1}{c}{deg$^2$} &         &  (Vega)           \\ \hline
Large Area Survey         & 190     & YJHK        & 18.2 \\
Galactic Clusters Survey  &  52     & ZYJHK       & 18.2 \\
Galactic Plane Survey     &  77     & JHK(+H$_2$) & 18.1 \\
Deep ExtraGalactic Survey &  3.1    & JK          & 20.7 \\
Ultra Deep Survey         &  0.8    & JK          & 21.6 \\
\hline
\end{tabular}
\caption{\it Depth and coverage in fields which have the full filter complement
in UKIDSS DR1}
\end{table}

% KNOWN PAPERS SO FAR
% Hewett, Lawrence, Dye, Warren
% Casali, Irwin, Hambly, Hodgkin
% Cirasuolo, Foucaud, McLure
% Lane, Simpson, Van Breukelen
% Lodieu a,b, Venemans, Warren07



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%               SURVEY COMPONENT SCIENCE CASE
%  UKIRT guidance for overall science case : <= 8 pages including figures
%  survey specific case : 7 pages 
% 
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\section{The Galactic Clusters Survey (GCS)}

\subsection{Introduction : original science case}

Broadly speaking, the process of star formation (SF) is now reasonably well
understood in terms of hierarchical fragmentation of collapsing
molecular clouds (Levy \& Lunine~1983; Mannings, Boss \& Russell~2001).
In detail, however, there is no complete picture of SF (Shu et al.~1987).
In particular, the spectrum of masses resulting from
the SF process, commonly known as the initial mass function (IMF), is 
difficult to predict. This is unfortunate, because the IMF is a fundamental 
tool
in studies of galaxy formation, stellar birthrate (Miller \& Scalo~1979), 
the chemical evolution of galaxies (Cameron~1993)
and the contribution of substellar objects to the
total mass in stellar systems (Hambly, Knox \& Hawkins~1999a). 
This last point is particularly 
interesting, since brown dwarfs (BDs; $m<0.08{\rm M}_{\odot}$) have
relatively high mass--to--light ratios at large ages and are not easily
observed. It is only recently that small--scale, deep infrared
studies have begun to tackle the question of the form of the very low mass 
IMF.

Since the pioneering work of Salpeter~(1955), there have been many 
determinations
of the MF for various stellar clusters and associations reaching ever lower
masses. In restricted mass ranges, MFs have usually been modelled using
power law forms after Salpeter, but the classic IMF
determination of Miller \& Scalo~(1979) shows a flattening of the
function at low masses and a log--normal model was fit over the full range
of data -- this has also been shown to be appropriate, for example, in
the Pleiades (Hambly et al.~1999b). More recent data show a flat, slowly
rising or slowly decreasing MF in the substellar r\'{e}gime
(e.g.~Lucas \& Roche~2000; Mart\'{\i}n, Zapatero--Osorio \& Rebolo~1998), 
and it is now
clearly important to firmly establish the form of the MF in as many
clusters as possible, with good statistics, to build upon these 
results. The possibility that free--floating planetary mass objects
exist (Lucas \& Roche 2000; Zapatero--Osorio et al.~2000), 
and if so, their relation to the `exoplanets' being
found in increasing numbers (see \verb+http://exoplanets.org+), 
are related questions that can be
tackled given sufficiently deep survey data. 

Theoretical predictions of the form of the IMF have advanced considerably 
over the last decade or so. Simple scaling arguments predict power--law
forms of the IMF in a hierarchical fragmentation procedure 
(Zinnecker, McCaughrean \& Wilking~1993). On the other hand,
Adams \& Fatuzzo~(1996) concentrated on the following
compelling argument: in the limit that many independent physical variables
come into play in the SF process, then the central limit theorem dictates 
that the IMF should approach a log--normal distribution. This clearly
has important implications for normal distributions having characteristic
masses
$m\sim0.1{\rm M}_{\odot}$ (e.g.\ Hambly et al.~1999b; Adams \& Fatuzzo~1996)
since the number of BDs predicted
at $m\sim0.01{\rm M}_{\odot}$ becomes very low (see later) relative to 
power--law forms with all except the most negative exponents. There is
currently not enough observational data in the substellar r\'{e}gime 
with which to confront such interesting theories. Furthermore,
theoretical predictions (e.g.\ Burrows et al.~1997; Chabrier et al.~2000) 
of the temperature and luminosity of
very low mass objects as a function of age have become much more secure 
over the last few years with the incorporation of non--gray atmospheric
models and dust. These advances are timely, since we can now predict,
with some confidence, the infrared absolute magnitudes and colours of
very low mass objects. This is of course pivotal in the derivation of
the mass function from observables.

The GCS aims to {\em measure} the substellar MF in a number of clusters and 
associations to masses $m\sim0.01{\rm M}_{\odot}$ ($\equiv$10M$_{\rm JUP}$,
units of Jupiter masses) in order to provide a firm footing for
theoretical models and more general Galactic studies. By measuring the MF in
a number of Galactic environments and at a range of different ages, we
aim to study the evolution of the MF over time, its relation to the IMF,
and the universality (or otherwise) of this fundamental tool of stellar
astrophysics.

The advantages of using clusters/associations for determining the IMF are
many, especially when compared to studies of the general field
population (e.g.\ Liebert et al.~2000). 
A cluster presents a single coeval population of stars
whose global properties (e.g.\ distance, age, metallicity) are known, in
some cases very accurately, via independent means. This is in stark 
contrast to the field populations, whose complex dynamical evolution and
star formation history makes measurement of the MF very difficult and 
derivation of the IMF almost impossible. 

The requirements for this programme are a selection of clusters/associations
with: small distances (to allow investigation of the least luminous and
therefore lowest mass objects); a good spread in ages (to allow investigation
of temporal evolution of the MF and inference of the IMF); and a variety
of Galactic environments (to allow investigation of the universality of the
IMF). Such a sample is presented in Table~1, with explanation in the caption,
and this is the UKIDSS GCS target list.
In order to predict the mass limits achievable we have used the DUSTY models
of Chabrier et al.~(2000), interpolating/extrapolating where required. While
some of these numbers are necessarily uncertain, they give an estimate of the
mass limits achievable. The numbers of BDs expected given certain assumptions
about the form of the mass function are also given. Here, we have assumed
for the sake of argument a universal MF based on that measured in the
Pleiades (e.g.\ Mart\'{\i}n et al.~1998; Hambly et al.~1999b) 
with various extrapolations to low masses. The normalisation
is to the total mass estimate for the cluster/association. 
In order to provide estimates of the numbers of BDs expected in the GCS
we have used two model forms along with data from the
Pleiades (e.g.\ Mart\'{\i}n et al.~1998; Hambly et al.~1999b). 
For power--law MFs we assume $\alpha=2.35$ for 
$m>0.5{\rm M}_{\odot}$; $\alpha=1.5$ for $0.5>m/{\rm M}_{\odot}>0.1$; and
the plausible values $\alpha=+1,0,-1$ for $m<0.1{\rm M}_{\odot}$. For the
log--normal, we assume a shape extrapolated from that measured in 
Hambly et al.~(1999b) and Moraux et al.~(2005). In each
case, the MFs are normalised to give the total mass estimated for each
cluster in Table~1.

In order to be
able to disentangle age/metallicity/environment effects and to quantify
evolutionary effects as the IMF translates into the present--day MF, we feel
that 10 targets is close to a minimum requirement. Assuming that these targets
are representative of the birthplace of most Galactic disk stars, this study
will yield information applicable to the Galactic disk as a whole. 
%Follow--up
%observations may include studies of the binary fraction and searches for
%eclipsing BDs that will confront theoretical models with real data.
Photometric identification of candidates requires multi--colour
measurements: various two--colour
diagrams are needed to measure reddening and hence extinction before
transformation of luminosity to mass; K photometry is useful for detecting
very young sources via hot dust emission. Proper motion measurements are
highly desirable to refine membership lists selected by photometry
alone since some cluster non--members will inevitably contaminate regions of
colour--magnitude and colour--colour diagrams where the cluster members
are found. All the regions surveyed will
be revisited in the K band for proper motion measurement over a 5~yr baseline.
%(see Appendix~\ref{gcsapp2})
(second epoch observations will also enable detection of 
Young Stellar Objects from K--band variability).

\begin{figure}
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\subsection{Progress in the GCS survey}

The GCS has progressed well in the first two years of UKIDSS. All high
priority targets have been observed in ZYJHK, with lower priority targets
being observed in K only to provide first epoch position measures for
proper motions. For more details, see the technical case below.


\subsection{Case for completion of the GCS}

%- continuing valdity of general goals

Needless to say, substellar MF research has progressed significantly in the
years since the original proposal submission (Spring~2001). The current
status of research is comprehensively illustrated in the proceedings of the
recent conference on ultra--low mass star formation which took place in
July~2005 (Mart\'{\i}n \& Magazz\`{u}~2005). Major advances are being made in
a number of areas, including surveys in far--infrared and submillimeter
wavelength ranges made possible by new technology (e.g.\ Greaves~2005;
Kauffman et al.~2005); computer simulations, for example in both 
stellar/substellar/planet formation (e.g.\ Thies et al.~2005) and
dynamical simulations of cluster evapouration (e.g.\ Goodwin et al.~2005);
evolutionary models (e.g.\ Fortney et al.~2005) and atmospheric models
(e.g.\ Reiners et al.~2005); and improvements in understanding of the
underlying astrophysics of substellar objects and their formation (e.g.\
Pavlenko et al.~2005; Whitworth \& Goodwin~2005; Wuchterl~2005). A natural
question to ask is: has the UKIDSS GCS programme been overtaken by other
surveys in the interim? The answer is a resounding `no'! Cluster
observations continue to be incremental in nature, as dictated by the
simple fact that it is almost impossible to secure sufficient observing
time on 4m--class facilities to execute a complete survey of a single
target, let alone the set of targets required to ensure a uniform and
unbiased study. Often, work is done in the optical on 2m--class
telescopes with relatively low areal coverage, and large extrapolations
are made which are severely hampered by statistical errors and are prone
to systematic errors from a highly uncertain level of contamination.
Typically, only two colours at a single epoch are used in the primary 
sample selection and no proper motion selection is possible.
This results in reddening being impossible to correct for; 
Gonz\'{a}les--Garc\'{\i}a et al.~(2006) is an example of the work
that continues to appear in the literature. Note that 2MASS lacks the
depth to probe the lower mass substellar sequences of the nearby star
clusters and star formation regions.

%- future goals

%- revised strategy

At a meeting of the GCS Working Group in Cambridge, 9~July 2003, revision
of the original GCS observational programme was discussed and agreed given
new information concerning the likely excellent short wavelength performance of
WFCAM and the advent of the UK joining ESO. The total time 
requirement was unaffected by this; the changes were made within the
existing time as originally proposed. The main changes were as 
follows:
\begin{itemize}
\item A re-examination of the original target list in the light of the UK 
joining ESO resulted in the most northerly target (M39) being dropped in
favour of an equatorial one (IC4665) to allow follow--up from Chile;
\item The WG revised the filter coverage, trading off area covered in
several of the larger targets for a wider wavelength baseline via inclusion
of ZY in addition to JHK (this decision has proved to be a good one as
demonstrated in the colour--magnitude diagram below).
\end{itemize}
For much more detail, see 
\verb+http://www.roe.ac.uk/~nch/gcs/new2yr/new2yr.html+ which is the
UKIDSS GCS WG web page.

%- detailed case, example science outcomes etc

The expected scientific return from the GCS is illustrated in the first two
refereed papers to be published from the survey (Lodieu et al.~2006a; 2006b).
In particular, Lodieu et al.~(2006a) demonstrate
\begin{itemize}
\item the power of the GCS multicolour approach in selecting clean cluster
membership samples;
\item the quantifiable completeness and reliability of the survey;
\item the promise of additional proper motion selection.
\end{itemize}
The first point is particularly important. As stated above, in other work
very often optical selection in two colours is used with subsequent IR 
follow--up from pointed observations. In the low S/N substellar r\'{e}gime
of such studies, the combination of higher reddening and photometric
scatter makes it very difficult to quantify completeness since cuts on
colour have tended to be tuned to yield samples that can be feasibly
followed up. In the GCS, on the other hand, we can choose the primary
colour--magnitude (CM) selection plane; Z versus Z--J produces excellent
separation between the cluster substellar sequence and non--members for
young star formation regions, e.g.~in Upper Sco (Figure~3 in Lodieu et
al.~2006a) and Orion (Figure~\ref{sigori} in this proposal). Of course,
this is not always the case especially for older targets in crowded
regions, but the availability of five--colour photometry and
proper motion selection allows us to weed out contaminating non--members,
making appropriate allowance for photometric errors in colour. Note that
even in Upper Sco, where a clear sequence is defined, we found that
$\sim25$\% of sources initially selected in the Z, Z--J CM plane (Figure~3
in Lodieu et al.~2006a) turned out to be non--members and this can
dramatically affect the slope of the derived MF. Moreover binarity,
which is often neglected in small scale experiments, can be studied
in different magnitude ranges by use of that CM plane where the locus of
the sequence of members is the shallowest.

\begin{figure}
\setlength{\unitlength}{1mm}
\begin{picture}(160,90)
\centerline{\special{psfile=orion.eps angle=0 hoffset=-110 voffset=-15 
hscale=40 vscale=40}}
\end{picture}
\caption{\em Z versus Z--J coloour--magnitude diagram for the Orion star 
formation central region ($\sigma$--Orionis)
in the UKIDSS DR1+ database (Warren et al.~2006). A clear substellar
sequence, extending to $m\sim10$M$_{\rm JUP}$ sits above the the general 
field population.}
\label{sigori}
\end{figure}

Hence, we assert with some confidence that the GCS programme as instigated in
the first two years of UKIDSS will achieve the desired aim of a uniform
census of the substellar present day MF in a variety of Galactic environments,
providing data to enable analysis of the underlying initial MF via accurate
quantification of the effects of completeness, binarity, reddening etc.\ to
provide an unparalleled dataset with which to critically confront 
state--of--the--art models of formation and evolution of brown dwarfs.


\subsection{Comparison with other surveys}

%- complementary proposals and how groovy it will all be

%- competing proposals and why this one is better

Moraux, Bouvier \& Clarke~(2005)
present a study that is perhaps the closest to the UKIDSS GCS in terms of
scope. However, the age range of the (smaller) list of targets is
limited and the mass range covers only the highest mass brown dwarfs.
Photometric identification of candidates primarily comes from optical (RIZ)
photometry with very low signal--to--noise in the substellar r\'{e}gime
and both completeness and contamination in this important mass range is a
significant concern. Because the MF is based on applying a steep 
mass--luminosity relationship to counts of cluster candidates (i.e.~the
luminosity function), the MF so derived is extremely sensitive to the
level of completeness and contamination at the faint end. It is only
via a large scale, homogeneous, multi--colour, multi--epoch infrared
survey that such concerns can be addressed accurately, and this is
precisely what the UKIDSS GCS has set out to achieve. 


%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
%               TECHNICAL CASE
%  UKIRT guidance : 1 page 
%
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\section{TECHNICAL CASE}  \label{TechCase}

\subsection{UKIDSS implementation}

The general principles of UKIDSS implementation are described in Lawrence \et\ (2006), and details relevant to each release are specified in Dye \et\ (2006) and Warren \et\ (2006). UKIDSS operates within the context of a working observatory (UKIRT) and dataflow system (VDFS), with the consortium taking quite specific roles. Survey design (fields, areas, filters, depths, and time required) is debated across the whole consortium in order to allow compromises between survey components. The overall survey design is summarised in Table 1 of Lawrence \et\ (2006) and at http://www.ukidss.org. Implementation (exposures, microstepping, jittering, seeing requirements, sky requirements) varies between survey components, and is the responsibility of working group heads, who enter MSBs in a database for queued action. (The specific implementation for GCS is described below). However, there is a standard unit of 40 second exposures, which is the best compromise between observing efficiency and survey rate, as described in Lawrence \et\.  The calibration plan has a dedicated working group. Calibration is based on 2MASS stars, tied to UKIRT faint standards. Observing is staffed in a series of short runs, by a significant fraction of the consortium. Quality Control filtering, and assistance to VDFS with production of merged and stacked survey products, is undertaken by a relatively small number of core working group members.  

From pipeline output over a year of data we now have an accurate assessment of actual achieved sensitivity, and it is close to the target depth. At 5$\sigma$, for point sources, using a 2" aperture magnitude, the standard 40second exposures give Y=20.2, J=19.6, H=18.8, and K=18.2. However, the rate of progress (sq.deg. surveyed per night) has been considerably less than hoped. On average across all the surveys, the rate of progress has been 79\% of that estimated in the proposal, and summarised in Table 1 of Lawrence \et\. In addition, the QC process has rejected 20\% of collected data. Most of the reasons behind both the lower efficiency and rejection rate are well understood and to a considerable extent have already been improved or corrected (e.g.\ faster PCs for data acquisition, avoidance of moon ghosts). We estimate that from here on efficiency will be 90\% of the original estimate, and QC will reject 10\% of data. As a result, to estimate nights needed for survey completion, we use the original models, but multiply by 1/0.8.  The number of years needed depends of course on the amount of WFCAM-UKIDSS time available per year, which currently is roughly half of all UKIRT nights. This is a matter for Board decision, but we note here that we have entered into negotiation with the University of Hawaii, which could potentially increase the number of UKIDSS nights per year by 20\%.

\subsection{Completion of GCS}

%- keep this short ; state that design is as in Lawrence et al but with following variation..

%- short few words about dithering, microstepping etc

%- estimated nights required : do this in simple minded way ..don't start afresh..

%(1) start with nights needed as quoted in Lawrence et al (2) Multiply by 1/0.8 for difference between expected efficiency and real efficiency (3) Scale according to any agreed changes in area, depth (4) quote REVISED TOTAL NIGHTS (5) estimate fraction done up to end of 2yr plan (May 2007) (6) quote NUMBER OF NIGHTS FOR COMPLETION.

This proposal seeks time to complete the GCS programme as originally
proposed, but with the (small) modifications discussed previously,
given the continuing validity of the science
case as demonstrated above. We request observing time to complete
ZYJHK imaging with second epoch coverage in the~K band as detailed
in Table~\ref{request}. Exposure times total 40s in all filters,
comprising 20s$\times$2 dithers in ZY, 10s$\times$4 dithers in JH and
5s$\times$2 dithers$\times2\times2$ microsteps in K for optimal relative
astrometry.
%Completion of the observational programme,
%as originally stated, is vital to provide good statistics in the
%lowest mass bins of the MFs in the range of targets in order to
%be able to make statistically meaningful statements as to the 
%universality (or otherwise) of the substellar IMF.

\setcounter{table}{2}
\begin{table}[h!]
\begin{center}
\begin{tabular}{crrr}
\hline
Target & \multicolumn{1}{c}{Fractional completion} & 
 \multicolumn{1}{c}{Revised total nights} & 
 \multicolumn{1}{c}{Nights required to complete} \\
       & \multicolumn{1}{c}{anticipated (2yr)} & &  \\
\hline \hline
\multicolumn{4}{c}{ }\\
IC~4665        &  83\% &  0.27 &   0.046 \\
Pleiades       &  83\% &  6.80 &   1.156 \\
Alpha Per      &  83\% &  4.35 &   0.740 \\
Praesepe       &  83\% &  2.45 &   0.417 \\
Taurus--Auriga &   9\% & 18.88 &  17.181 \\
Orion          &   8\% & 13.32 &  12.254 \\
Upper Sco      &  12\% & 13.32 &  11.722 \\
Perseus OB2    &  83\% &  1.09 &   0.185 \\
Hyades         &  17\% & 25.15 &  20.875 \\
Coma Ber       &  12\% &  6.80 &   5.984 \\
\multicolumn{4}{c}{ }\\
             & TOTALS: & 92.43 &  70.560 \\
\multicolumn{4}{c}{ }\\
\hline
%\multicolumn{4}{l}{$^1$assuming total observing efficiency 0.8 (taking into
%account DQC losses of 0.1)}
\end{tabular}
\caption{\em Observing time request for completion of the UKIDSS GCS to the
full programme, in priority order. Fractional completeness is as anticipated
at the end of the 2 years; revised totals assume efficiency 0.8 with
respect to figures in Lawrence et al.~(2006).}
\label{request}
\end{center}
\end{table}





%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
%               DATA MANAGEMENT
%  UKIRT guidance : 1 page 
%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{DATA MANAGEMENT}  \label{DataMgt}

Data Management for UKIDSS employs the VISTA Data Flow System (VDFS).
Data frames are transported to the Cambridge Astronomical Survey Unit (CASU) 
where they are processed using the VDFS pipeline. Processed frames and per-frame
catalogues are sent over the internet to the Edinburgh Wide Field Astronomy Unit 
(WFAU) where they are ingested into the WFCAM Science Archive (WSA). 
The final stages needed to produce UKIDSS survey products - 
Quality Control (QC) filtering,
stacking, mosaicing, and band-merging - are the joint responsibility
of UKIDSS members and VDFS project staff. Although implementation
is shared, the UKIDSS consortium
has prime responsibility for design of the QC processes and algorithms.
UKIDSS and the VDFS projects have had an intimate relationship throughout 
their histories; several members of the VDFS
project are also UKIDSS members, and the UKIDSS consortium was used, through
the `twenty questions' method to produce the Science Requirements Analysis Document 
for VDFS. Most of the structure of both the pipeline and the science archive
was designed explicitly with UKIDSS in mind.   
Our aim is to release UKIDSS data products in a staged manner, roughly
every six months. Again, this is done in a carefully agreed collaborative
procedure with the VDFS project. To date, we have made two releases - the 
`Early Data Release (EDR)' on Feb 10th 2006, and `Data Release 1 (DR1)' 
on July 21st 2006. Each was accompanied by a `data release paper' 
specifying in detail the technical parameters of the dataset released 
(Dye \et\ 2006; Warren \et\ 2006; available on astro-ph and at 
http://surveys.roe.ac.uk/wsa/pubs.html .


%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
%               COLLABORATORS and INSTITUTIONS
%  UKIRT guidance : 1 page 
%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{COLLABORATORS and INSTITUTIONS}  \label{Collabs}

This proposal is submitted by the {\em UKIDSS Consortium}. 
This is a consortium of over 100 individual astronomers across
Europe, whose purpose is to implement the UKIRT Infrared Deep Sky Survey,
in collaboration with the Joint Astronomy Centre (who operate WFCAM on UKIRT), 
and the VISTA Data Flow System project, who produce the WFCAM Science Archive.
The aim of the UKIDSS consortium is to produce the scientific design for
the survey; to win the telescope time necessary; to plan the implementation of
the survey, liaising with the other bodies above; to staff the
observing implementation; to define the necessary Quality Control (QC) filtering stages 
to produce final survey products; to assist the data processing team as necessary
in producing stacked and merged survey products; and finally to document the
production of the survey data in scientific publications and other technical papers.
 
The consortium holds no proprietary data rights, and is open to any
European astronomer to join. The current membership is listed at http://www.ukidss.org/consortium/consortium.html  
UKIDSS is operated through a set of working groups, whose Heads
constitute an informal executive body in frequent contact. The key
figures within the consortium are currently : 

\footnotesize
\begin{verbatim}

Consortium Principal Investigator (CPI)     Andy Lawrence      Edinburgh
Consortium Survey Scientist (CSS)           Steve Warren       Imperial College
Head of Large Area Survey (LAS)             Richard Jameson    Leicester
Head of Galactic Plane Survey (GPS)         Phil Lucas         Herts
Head of Galactic Clusters Survey (GCS)      Nigel Hambly       Edinburgh
Head of Deep Extragalactic Survey (DXS)     Alastair Edge      Durham
Head of Ultra Deep Survey (UDS)             Omar Almaini       Nottingham
Head of Pipeline and Archive Group          Steve Warren       Imperial College
Head of Calibration Group                   Paul Hewett        Cambridge
Head of Implementation Group                Steve Warren       Imperial College
 
\end{verbatim} 
\normalsize


%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% example of figure
% FIGURE : GENERAL GOALS : SURVEY DEPTH COMPARISON


%\begin{figure}

%\includegraphics[width=90mm,angle=0]{surveys.eps}

%\caption{\it Illustration of the scope 
%of the five UKIDSS survey components,
%and their sum, 
%by comparison with 2MASS. The comparison is made in terms of expected number of 
%photons and effective volume, for the K band, computed as described in the text}

%\end{figure}

%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%



%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%    REFERENCES
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\newpage

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\end{document}
