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Astron. Astrophys. 322, 455-459 (1997) 2. Observations and reductionsAll observations for this program were obtained at the 2.56 m
Nordic Optical Telescope (NOT), La Palma. The observed area covers 180
The I data was taken with BROCAM1 (TEK1K), operated in
cassegrain focus with 0.176"/pixel and 3'x3' field. For future proper
motion measurements, the astrometry errors due to nonuninform pixels
and possible effects of rotator position were reduced by using four
different position angles for each I-field (0, 90, 180 and 270
degrees) exposing 5 min at each position. Debiassing and flatfield
corrections were done in a standard fashion within IRAF (Image
Reduction and Analysis Facility)
1. Median seeing was
The JK observations were done with the ARNICA NICMOS3
(256x256) array, which was made available at NOT via a collaboration
with Arcetri Astrophysical Observatory, Florence. The last third of 6
nights in Aug-Sep95 was used. Unfortunately the pixel size (0.55") was
not very well matched to the seeing ( The J data could be treated the same way as I, but high and rapidly varying background in K necessitated a different approach. The sky for each K -image was defined as the median of the four images nearest in time and subtracted from the image, which then was flatfielded by a differential flat. 2.1. Classification of objectsA major problem in this kind of survey is to distinguish stars from
distant galaxies at faint magnitudes. The whole area was visually
inspected and all objects were classified as stars, galaxies, binaries
or unclassifiable (too faint for a meaningful classification). 1411
objects out of 3800 were classified as stars. Since the seeing
conditions were excellent it is estimated that the discrimination
between stars and galaxies is reliable to 2.2. PhotometrySince point spread functions (PSFs) were undersampled in JK it was not suitable to use ordinary PSF fitting. For single aperture photometry it is necessary to always keep the same aperture radius. However for the JK data centering errors and focus shifts are non-negligible, thus in order to maximize the signal to noise ratio it was desirable to change aperture radius from one object to another. A new, more robust, method (used also in I) was developed, brief outlines: 1. All objects were measured in a series of 80 apertures, with radii ranging from 0.05" to 4" in steps of 0.05". 2. From the "best" stars in each field a growth curve (Stetson 1990) was constructed, i.e. magnitude shift as function of aperture radius. 3. Each objects' curve was subtracted by that frames' growth curve.
Ideally this curve is completely flat, but due to centering errors,
errors in the sky level etc... that is generally not the case.
However, there is normally an almost flat part of the curve at
Transformation of JK instrument magnitudes to the CIT system
was done by observations of IR standard stars and transformation
equations provided by the ARNICA team (Hunt et al. subm.). I
instrument magnitudes were transformed to the Kron-Cousins system via
observations of Landolt (1992) standard stars. Typical internal errors
are 0.1 mag ( Table 1. Photometry of potential Pleiades members. Magnitude errors are internal. Table 2. The number of Pleiades candidates in the magnitude interval Table 3. M-dwarf candidates, including the Pleiades candidate NOT1. Magnitude errors are internal. Distance errors are of the order of 10%. All objects recognized as binaries or stars very close to a galaxy in I were, as a check, also measured by PSF-fitting. For a few objects that were resolved in I, but not in JK, the whole system was measured as one object in all bands, thus getting the binary system correct in the colour magnitude diagrams. 2.3. Completeness limitsIn this kind of surveys it is important to know the magnitude limit
to which the survey is complete. The number of detected stars as a
function of magnitude increases exponentially and gives a straight
line in a log( ![]() ![]() ![]() ![]() © European Southern Observatory (ESO) 1997 Online publication: June 5, 1998 ![]() |