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A guide to IRCS imaging exposure times Background-limited operation
In order to achieve the maximum sensitivity in a given integration time,
individual exposures should be long enough for the photon shot noise from
the sky background to dominate over the array read noise. In practice,
background-limited performance (BLIP) is considered to be when the sky
counts exceed the square of the read noise by a factor of 3.
Observations at L' and M' are background-limited even
in the shortest exposure time. The following tables assume use of the infrared
secondary mirror.
| Filter |
Background |
Min. BLIP time (s) |
| (mag/arcsec2) |
(e-/s/arcsec2) |
20 mas |
52 mas |
| J |
15.7 |
18 000 |
80 |
13 |
| H |
13.9 |
83 000 |
12 |
4 |
| K' |
14.1 |
40 000 |
30 |
5 |
| K |
13.7 |
52 000 |
20 |
5 |
| L' |
5.0 |
70 000 000 |
- |
- |
| M' |
1.8 |
200 000 000 |
- |
- |
Non-linearity of the camera detectorTo achieve less than
1% non-linearity, we recommand a maximum signal value less than 4000
ADU (= 22,400 e-) for a single exposure. For L' and M' bands imaging,
the signal level of 7000 ADU (= 39,200 e-) can be allowed with less
than 3% non-linearity because of very high background level. [non-linearity of camera detector]
Saturation magnitudes
The time it takes for a source to saturate is obviously dependent on the
seeing, which can be extremely good on Mauna Kea. The following exposures
times
should therefore be considered as a guide, and are based on 0.3'' seeing
for the 52 mas pixel scale, and Adaptive
Optics for the 20 mas pixel scale.
52 mas pixel scale
| Filter |
Saturation magnitude |
Max exp
time (s) |
| 1 s |
5 s |
10 s |
30 s |
60 s |
120 s |
300 s |
| J |
10.7 |
12.4 |
13.2 |
14.4 |
15.2 |
16.0 |
17.2 |
1000 |
| H |
10.6 |
12.3 |
13.1 |
14.4 |
15.4 |
16.6 |
- |
200 |
| K' |
10.0 |
11.7 |
12.5 |
13.7 |
14.6 |
15.5 |
17.4 |
420 |
| K |
9.9 |
11.6 |
12.4 |
13.7 |
14.5 |
15.5 |
18.4 |
330 |
| L' (1) |
|
0.20 |
(1) 512x512 pixel subarray.
20 mas pixel scale
| Filter |
Saturation magnitude |
Max exp
time (s) |
| 1 s |
5 s |
10 s |
30 s |
60 s |
120 s |
300 s |
| J |
11.3 |
13.0 |
13.8 |
15.0 |
15.7 |
16.5 |
17.5 |
6000 |
| H |
11.7 |
13.4 |
14.2 |
15.4 |
16.2 |
17.0 |
18.1 |
1300 |
| K' |
11.1 |
12.8 |
13.6 |
14.8 |
15.6 |
16.3 |
17.4 |
2800 |
| K |
11.0 |
12.7 |
13.5 |
14.7 |
15.5 |
16.2 |
17.3 |
2100 |
| L' |
|
0.62 |
| M' |
|
0.28 |
Shortest exposure times with sub-array sizes| Sub-Array Size | Readout Mode | Normal (sec) | Thermal (sec) | | 10242 (Full Array) | 0.41 | 0.119 | | 8962 | 0.33 | 0.096 | | 7682 | 0.26 | 0.076 | | 6402 | 0.20 | 0.058 | | 5122 | 0.14 | 0.042 | | 3842 | 0.10 | 0.029 | | 2562 | 0.06 | 0.018 | | 1282 | 0.029 | 0.009 | | 642 | 0.017 | 0.006 |
Overheads for thermal-infrared observations
The short integration times required at L'M' result in substantial
overheads.
| Observing mode |
Total required time |
| w/o AO |
[total itime] × 3 |
| w/ AO | [total itime] × 3 + [15-20min] per target for AO parameter adjustment(1) |
(1) If targets have similar magnitudes within 1-2 mag,
the AO parameter adjustment can be performed just a few times during
the observation in a stable seeing condition.
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