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<H1><A NAME="SECTION002910000000000000000">&#160;</A>
<A NAME="irspec-introduction">&#160;</A>
<BR>
Introduction
</H1>

<P>
IRSPEC is a cryogenically cooled grating spectrometer equipped with a
relatively small (for optical CCD standards)  2D array of
62x58 pixels. 
It covers the 1&nbsp;<IMG
 WIDTH="44" HEIGHT="70" ALIGN="MIDDLE" BORDER="0"
 SRC="img998.gif"
 ALT="$\mu$">m to 5&nbsp;<IMG
 WIDTH="44" HEIGHT="70" ALIGN="MIDDLE" BORDER="0"
 SRC="img999.gif"
 ALT="$\mu$">m
wavelength range and the two back-to-back gratings - #2 optimized for
observations at 
<!-- MATH: $\lambda\le2.5$ -->
<IMG
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 SRC="img1000.gif"
 ALT="$\lambda\le2.5$">&nbsp;<IMG
 WIDTH="44" HEIGHT="70" ALIGN="MIDDLE" BORDER="0"
 SRC="img1001.gif"
 ALT="$\mu$">m and #1 for longer wavelengths -
yield a dispersion of <IMG
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 ALT="$\simeq5$">
&#197;/pixel in H and K
(1.4-2.5&nbsp;<IMG
 WIDTH="44" HEIGHT="70" ALIGN="MIDDLE" BORDER="0"
 SRC="img1003.gif"
 ALT="$\mu$">m), <IMG
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&#197;/pixel in L,M (3-5&nbsp;<IMG
 WIDTH="44" HEIGHT="70" ALIGN="MIDDLE" BORDER="0"
 SRC="img1005.gif"
 ALT="$\mu$">m) while in J
(1-1.3&nbsp;<IMG
 WIDTH="44" HEIGHT="70" ALIGN="MIDDLE" BORDER="0"
 SRC="img1006.gif"
 ALT="$\mu$">m) one can choose between <IMG
 WIDTH="64" HEIGHT="54" ALIGN="BOTTOM" BORDER="0"
 SRC="img1007.gif"
 ALT="$\simeq2$">
&#197;/pixel (grating #2 
order 2) or <IMG
 WIDTH="10" HEIGHT="21" ALIGN="BOTTOM" BORDER="0"
 SRC="img1008.gif"
 ALT="$\simeq3.5$">
&#197;/pixel (grating #1 order 3). In all cases
the resolving power is quite high and each frame covers a small wavelength
range; obtaining complete spectra of an atmospheric window requires
<IMG
 WIDTH="46" HEIGHT="54" ALIGN="BOTTOM" BORDER="0"
 SRC="img1009.gif"
 ALT="$\sim$">20 images at different grating positions.
Along the slit the pixel size is <IMG
 WIDTH="10" HEIGHT="21" ALIGN="BOTTOM" BORDER="0"
 SRC="img1010.gif"
 ALT="$\simeq2.2$">
arcsec and the total,
usable slit length is slightly less than 2 arcmin; small areas at the edges
of the slit are vignetted. 

<P>
Although there is no standard procedure for the observations, it is
generally agreed that the most convenient strategy to subtract the strong
sky emission - OH airglow up to 2.25&nbsp;<IMG
 WIDTH="44" HEIGHT="70" ALIGN="MIDDLE" BORDER="0"
 SRC="img1011.gif"
 ALT="$\mu$">m and thermal + molecular bands
beyond - is to alternatively measure the `object' and the `sky' and subtract
the frames (note that the `sky' frame may also be taken with the object
in another position along the slit). On chip subtraction of the sky emission
- - the procedure normally used for optical CCD's - gives worse results due
to the large intensity of the sky background combined with the relatively bad 
cosmetic quality of the infrared arrays.
The object-sky telescope nodding is typically done every few minutes and
one or more frames per telescope positions are produced and stored.
At the end of the night, therefore, one has collected several hundred images
which may also include data taken at many different wavelengths.
This document describes a few procedures (commands) developed
to make the handling of the many frames 
somewhat easier.
For each command I did my best to provide you with long and 
exhaustive help files which are available on line. Here I just briefly
describe the steps to follow to take full advantage of the commands
available (remember to type SET/CONTEXT IRSPEC to access them).

<P>
<BR><HR>
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<LI><A NAME="tex2html7594"
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<LI><A NAME="tex2html7595"
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<ADDRESS>
<I>Petra Nass</I>
<BR><I>1999-06-15</I>
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