Guide for IRCS Imaging Exposure Time Estimation
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 (mag/arcsec2) | Background (e-/s/arcsec2) | Min. BLIP time (s) 20 mas | Min. BLIP time (s) 52 mas |
---|---|---|---|---|
J | 14.7 | 41,300 | 20 | 5 |
H | 13.7 | 100,000 | 9 | 3 |
K' | 12.9 | 107,000 | 8 | 3 |
K | 12.4 | 165,000 | 6 | 3 |
L' | 2.6 | 520,000,000 | - | - |
M' | -0.1 | 740,000,000 | - | - |
Non-linearity of the Camera Detector
To achieve less than 1% non-linearity, the maximum signal counts should be 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.
Please see here for the detailed information of non-linearity.
Saturation Magnitudes
The time it takes for a source to saturate is obviously dependent on the seeing, which can be extremely good on Maunakea. The following exposures times should therefore be considered as a guide, which are based on 0.3'' seeing for the 52 mas pixel scale, and Adaptive Optics for the 20 mas pixel scale. These information are based on no-AO data.
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 |
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' and M'-bands result in substantial overheads.
Observing mode | Total required time |
---|---|
w/o AO | [total integration time] Γ 3 |
w/ AO | [total integration time] Γ 3 + 15-20min(1) |
(1) The time needed for AO parameter adjustment. If the targets have similar magnitudes within 1-2 mag, the AO parameter adjustment can be performed within a few times during the observation in a stable seeing condition.