There are two approaches that could be used:
I am opting for the latter. The primary advantage is that it ensures greater uniformity of calibration. Flat-fielding IRAC is already problematic due to variation in the sky. By selecting a finite number of flat-field locations we can pre-select these to ensure that they minimize the number of bright stars and offensive extended structure (such as significant cirrus).
To see what the other instruments have done, you can go to:
Selection
I have selected 24 points spaced at 15 degree intervals along the ecliptic. This ensures that there is one spot that is between 0 and 15 degrees away from the best location allowed. As many six of spots are visible at any one given time. The spacing between these points sets the maximum distance one can be from the ideal point. However, we don't want to make them too close or we will have defeated the whole point of having a finite number in the first place. Conversely, they must be no more than 40 degrees apart to ensure visibility. A 15 degree shift from the "best" location is roughly a drop of 20% in intensity, and seems like a good compromise.
Furthermore, after talking to Jeonghee I have shifted the points 5 degrees off the ecliptic itself to try and avoid zody structure. This is a small loss in intensity of a few percent.
I then examined the ISSA plates using the visualization tool in SPOT and chose either the plus or minus 5 degree position based on the number/flux of 12um sources and the degree of cirrus structure seen at 100um. In some cases I tweaked the positions further to better optimize them for the above. Note that I have not looked at the 2MASS data for these regions yet to further optimize them. Volunteers?
| Name | Eclip. Long. | Eclip. Lat. |
| zody_field_1 | 0.00 | -5.00 |
| zody_field_1 | 0.00 | -5.00 |
| zody_field_2 | 15.00 | -5.00 |
| zody_field_3 | 30.00 | -5.00 |
| zody_field_4 | 45.00 | +5.00 |
| zody_field_5 | 60.00 | -5.00 |
| zody_field_6 | 75.00 | +5.00 |
| zody_field_7 | 90.00 | -5.00 |
| zody_field_8 | 105.00 | +5.00 |
| zody_field_9 | 120.00 | -5.00 |
| zody_field_10 | 135.00 | -5.00 |
| zody_field_11 | 150.00 | -4.00 |
| zody_field_12 | 165.00 | -5.00 |
| zody_field_13 | 180.00 | +5.00 |
| zody_field_14 | 195.00 | +5.50 |
| zody_field_15 | 210.00 | +7.00 |
| zody_field_16 | 225.00 | -5.30 |
| zody_field_17 | 240.00 | +5.00 |
| zody_field_18 | 255.00 | -5.20 |
| zody_field_19 | 270.00 | +5.00 |
| zody_field_20 | 285.00 | +5.00 |
| zody_field_21 | 300.00 | -7.00 |
| zody_field_22 | 315.00 | -5.80 |
| zody_field_23 | 330.00 | +4.30 |
| zody_field_24 | 345.00 | +5.00 |
Table with FITS images for all of the above fields.
Scheduling
The in-flight procedure would then be as follows:
The AORs for the above are attached here. Note that these are the 3x3 (9 dither) pattern planned for the mask-and-coadd reduction and which was prototyped previously. Also included at the end is the aor for the NEP dark which goes along with this observation. I expect to take the flat and it's own dark back-to-back. The regular sky dark does not take as many images as this special dark, and hence would be a noticeable contributor to the noise in the derived flat. I have yet to figure out with the OPS group how we will specify the constraints.