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Instrument Evolution |
This page contains information about the time evolution of various instrumental
parameters, such as the RON, the number of bad pixles, the gain, the throughput.
If you have data that can be relevant to these issues please e-mail them to
us, it will help us to monitor the instrument performance.
Detector Characteristics
Instrument Throughput, Atmospheric
Extinction and Filter Transformations
Focus Pyramid
Collimator Focus Positions
Encoder Positions
Detector Characteristics:
Read-out Noise : Last values (Unit : ADU)
| Date \ Qaudrant |
Lower Left |
Lower Right |
Upper Left |
Upper Right |
| Nov 16 2002 |
2.439 |
2.094 |
2.097 |
2.131 |
Read-out
Noise evolution since January 1998
Gain : Last value (Unit : e-/ADU)
| Date |
Gain |
| Nov 22 2002 |
5.267 |
Gain evolution since August
1998
Non-Linearity
| Month |
Gain |
Nov 2002
|
Less than 1.5% between 50 and 10000 ADUs |
Bad pixels
Last
values :
| Date |
Dead pixels |
Hot pixels |
Noisy pixels |
Total bad pixels |
| Nov 1999 |
170 |
1406 |
negligeable |
1580 |
go to the bad pixel image
Instrument Throughput, Atmospheric Extinction and
Filter TransformationImaging Modes
Zero Points
| Imaging mode and filter |
J - LF |
H - LF |
Ks - LF |
Z - LF |
J - SF |
H - SF |
Ks - SF |
J - SO |
H - SO |
Ks - SO |
Ks - HRF |
J - LF_FE |
Ks - LF_FE |
| Zero Point |
22.97 |
22.86 |
22.31 |
22.60 |
23.34 |
23.03 |
22.50 |
22.94 |
22.86 |
22.34 |
22.32 |
23.14 |
22.38 |
| Date of last measure |
Feb 2002 |
Feb 2002 |
Feb 2002 |
Dec 1997 |
May 1998 |
May 1998 |
May 1998 |
Jan 2002 |
Jan 2002 |
Jan 2002 |
Dec 1997 |
Jul 1998 |
Jul 1998 |
Atmospheric Extinction
| Date \ Filter |
J |
H |
K |
Ks |
| La Silla Folklore |
0.08 |
0.06 |
0.11 |
|
| October 98 |
0.10 |
0.04 |
|
0.05 |
| March 00 |
0.08 |
0.03 |
|
0.05 |
Filter Transformations
In the following, lower case refer to SOFI instrumental magnitudes' corrected
for atmospheric extinction and upper case letters refer to tabulated magnitudes
in the Persson et al. list of standards. Stars in the J-Ks colour range 0.24
to 1.28 were used to derive the following relationships.
- J-j=-0.007(J-K)+23.15, fit residual 0.013 magnitudes
- H-h=-0.022(J-K)+22.98, fit residual 0.009 magnitudes
- Ks-ks=0.023(J-K)+22.38, fit residual 0.013 magnitudes
- K-ks=-0.005(J-K)+22.39, fit residual 0.017 magnitudes
These results are preliminary and a more detailed analysis, including errors,
will be listed soon.
Spectroscopic Modes
Counts are in electrons per second per Angstrom for a 15th magnitude A0
star at Zenith.
| Date \ Grism-Wavelength |
Blue 10500 |
Blue 12000 |
Blue 13000 |
Blue 15000 |
Red 16000 |
Red 17000 |
Red 22000 |
Red 23000 |
Red 24000 |
| March 1998 |
4.5 |
3.8 |
2.9 |
1.9 |
1.7 |
1.6 |
1.1 |
0.83 |
0.61 |
Focus Pyramid
The distance "d" between the four outlying images produced by the focus
wedge and the central image and the telscope defocus "f" are linearly related
by d=a+b*f. Errors in the co-efficients are in brackets.
| Date\Co-efficients |
a |
b |
| December 1997 |
35.2 |
-15.4 |
| March 1998 |
35.1 |
-14.4 |
| May 1998 |
35.1 |
-16.4 |
| July 1998 |
34.95 (0.12) |
-15.5 (0.5) |
| August 1998 |
35.21 (0.09) |
-16.8 (0.4) |
| September 1998 |
35.11 (0.11) |
-14.9 (0.4) |
| January 1999 |
35.05 (0.10) |
-14.9 (0.3) |
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Collimator Focus
| Imaging mode |
Date of last test |
Ks |
H |
J |
Z |
NB_1.061 |
NB_1.187 |
NB_2.090 |
NB_2.195 |
NB_HeI_J |
NB_1.215 |
NB_FeII_J |
NB_Pbeta |
NB_FeII_H |
NB_1.71 |
NB_HeI_K |
NB_H2_S1 |
NB_Brgamma |
NB_CO |
NB_2.248 |
NB_2.28 |
| Large_field_imaging |
15Apr2000 |
2944 |
3293 |
1849 |
404 |
2436 |
3796 |
4708 |
4543 |
2826 |
3787 |
4914 |
4979 |
11793 |
5989 |
5168 |
7552 |
5216 |
4841 |
7411 |
5046 |
| Small_field_imaging |
22Jan2000 |
-2651 |
-2852 |
-4733 |
-1354 |
-1793 |
-1902 |
-1930 |
-2246 |
-1740 |
-1834 |
-486 |
-896 |
1788 |
-371 |
-1461 |
-1121 |
-1243 |
-1538 |
132 |
-1704 |
| Spectroscopic_Objective |
23Jan2000 |
2537 |
-295 |
-2596 |
-6254 |
-3190 |
-1482 |
2553 |
2813 |
-3021 |
-1098 |
-129 |
186 |
5562 |
2227 |
2580 |
3105 |
2661 |
2630 |
3892 |
1969 |
Grisms
The optimal focus for the grisms is determined by using the JG mask. I.e.,
the focus is determined for the best spatial resolution. In general, the position
of the collimator required to obtain the best spectral resolution is different
from the collimator position required for the best spatial resolution.
| Date\Grism |
Blue Grism |
Red Grism |
HR Z |
HR J |
HR H |
HR Ks |
| 980517 |
2000 |
0 |
|
|
|
|
| 990122 |
-1567 |
541 |
1294 |
2016 |
3924 |
5607 |
Wollaston
| Date\Filter |
Wollaston Lower (Ks) |
Wollaston Upper (Ks) |
| 980630 |
3883 |
2976 |
Encoder Positions
See the relavent SPC file on wsofi.
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