Table A.4.
Factors to convert the CIB intensity (in Jy/sr with the convention νIν = constant) into the HFI, ACT, and SPT bandpasses (see Eqs. (A.3) and (A.5)). ν1 and ν2 are given in the first column and first line, respectively (e.g. K(ν1, ν2) = K(857, 545) = 1.989.
| Planck/HFI | ACT | SPT | |||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| 857 | 545 | 353 | 217 | 143 | 100 | 148 | 218 | 277 | 95 | 150 | 220 | ||
| 857 | 1 | 1.989 | 5.712 | 24.155 | 97.650 | 269.51 | 83.00 | 25.50 | 12.43 | 294.03 | 75.08 | 25.62 | |
| 545 | … | 1 | 2.872 | 12.15 | 49.10 | 135.52 | 41.74 | 12.82 | 6.25 | 147.85 | 37.75 | 12.88 | |
| HFI | 353 | … | … | 1 | 4.229 | 17.10 | 47.18 | 14.53 | 4.465 | 2.176 | 51.48 | 13.14 | 4.485 |
| 217 | … | … | … | 1 | 4.043 | 11.16 | 3.436 | 1.056 | 0.5146 | 12.17 | 3.108 | 1.061 | |
| 143 | … | … | … | … | 1 | 2.760 | 0.8500 | 0.2612 | 0.1273 | 3.011 | 0.7688 | 0.2624 | |
| 100 | … | … | … | … | … | 1 | 0.3090 | 0.09463 | 0.046121 | 1.090 | 0.2786 | 0.09506 | |
| 148 | … | … | … | … | … | … | 1 | 0.3073 | 0.1498 | 3.542 | 0.9045 | 0.3087 | |
| ACT | 218 | … | … | … | … | … | … | … | 1 | 0.4874 | 11.53 | 2.944 | 1.005 |
| 277 | … | … | … | … | … | … | … | … | 1 | 23.66 | 6.040 | 2.061 | |
| 95 | … | … | … | … | … | … | … | … | … | 1 | 0.2553 | 0.08713 | |
| SPT | 150 | … | … | … | … | … | … | … | … | … | … | 1 | 0.3413 |
| 220 | … | … | … | … | … | … | … | … | … | … | … | 1 | |
Notes. The factors were computed using the Béthermin et al. (2012a) CIB SED. Some factors can be deduced from combinations of others. We give all of them for convenience.
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