This is an observation to look for the absorption lines of H3+, H2, and
CO along the line of sight to the Galactic center on the continuum of bright infrared
sources there. 1) Slit PA and nodding amplitude in order to make the most of the
telescope time, we set the slit position angle so that a nearby bright IR source
is also covered in the same slit, which may also serve as a decent background illumination
for the absorption line survey. We measured the slit P.A. as accurate as possible
using our own imaging at Mauna Kea, but, since the slit length of CRIRES is long,
there is chance that the sources are not precisely in the slit. In such a case,
we would appreciate if the observers could pay attention to the following possibilities
- small tweaking of the slit P.A. at the site, so that two source are properly
centered in the slit, - if this is not possible, we will put the priority to the
primary source (unambiguously addressed in OBs and finding chart). Please centerd
the primary source on the slit. In this case, a slight off-centering of the secondary
source is acceptable. 2) Centering objects on the slit Beacuse two sources are
to be covered in one slit, we would like to put the middle of the two sources at
the center of the slit, instead of putting the primary source at the center of the
slit. The offsets are shown in the finding chart, and also below. 3) Spectroscopic
standard
The order of the execution of each OBs is not very cretical, but the calibration
star HR 6879 is meant to be observed after the object (therefore earlier R.A.).
1) We revise the priority of the objects as follows (the smaller the number, the
higher the priority). Corresponding calibration stars are give same priority.
GCS3-2 H3P -> 1
IRS1W H3P -> 2
GCS3-1 H3P -> 3
GCS3-2 H2 -> 4
GCS3-2 CO -> 5
IRS1W CO -> 6
GCS3-1 CO -> 7
IRS16NE H3P -> 8
IRS16NE CO -> 9
All CAL -> 10
2) If it is possible, we would like to propose a small tweak for a grating setting.
The primary line we would like to cover by 27/1/i was H2 1-0 S(1) at 2121.8 nm.
It turns out, by using 27/1/n instead of 27/1/i,
we can still cover not only the original line of H2, but also another line of
H3+ as a genuine bonus. The order of the grating stays the
same (just for a change from "/i" to "/n"). The details of the line positions
and the margins at both sides of the lines are following.
[27/1/i l_ref = 2123.3 nm]
H2 1-0 S(1) at 2121.8nm/ H3+ tR(6,6) 2093.265nm
Det.1 covers 2093.1 - 2103.3 2093.265 -24km/s to +1437km/s
Det.3 covers 2118.6 - 2128.0 2121.8 -452km/s to +876km/s
[27/1/n l_ref = 2117.6 nm]
H2 1-0 S(1) at 2121.8nm/ H3+ t(6,6) 2093.265nm
Det.1 covers 2087.0 - 2097.4 2093.265 -897km/s to +592km/s
Det.3 covers 2112.8 - 2122.4 2121.8 -1272km/s to +85km/s
3) Vignetting problem
Our configuration lists are as follows for the target lines, wavelength,
detector number, and grating settings:
H3+
3533.67 R(3,3)l det3 16/0/n
3645.09 R(4,4)l det3 15/-2/n
3715.48 R(1,1)l det2 15/-1/i
2093.265 R(6,6) det1 27/1/n
H2
2121.8 1-0 S(1) det3 27/1/n
2223.5 1-0 S(0) det2 25/-1/n
CO
2356.12 P(4) N/A
2353.87 P(3) det4 24/-1/i
2351.67 P(2) det4 24/-1/i
2349.50 P(1) det4 24/-1/i
2345.31 R(0) det4 24/-1/n
2343.27 R(1) det4 24/-1/n
2341.28 R(2) det3 24/-1/i and det 4 24/-1/n
2339.32 R(3) det3 24/-1/i
2337.41 R(4) det3 24/-1/i
2335.54 R(5) det3 24/-1/i
2333.72 R(6) det3 24/-1/i and 24/-1/n
Dr. Michael Hilker (ESO) had already confirmed that our settings are fine
because the orders 25 and higher are affected in detector 4.