Table 2
Parameters used to fit the local ISRF with black-bodies.
T0[K] | Urad [10-11 GeV cm-3] | ||
|
|||
CMB | 2.726 | Planckian (b-b) | |
|
|||
M1 | IR | 33.07 | 25.4 (4.5 × 10-5 × b-b) |
|
|||
Stellar | 313.32 | 5.47 (1.2 × 10-9 × b-b) | |
|
|||
3,249.3 | 37 (7.03 × 10-13 × b-b) | ||
6,150.4 | 22.9 (3.39 × 10-14 × b-b) | ||
23,209.0 | 11.89 (8.67 × 10-17 × b-b) | ||
|
|||
M2 | IR | 33.653 | 32.12 (5.3 × 10-5 × b-b) |
|
|||
Stellar | 313.32 | 6.2 (1.36 × 10-9 × b-b) | |
|
|||
2,901.13 | 33.76 (1.01 × 10-12 × b-b) | ||
5,570.1 | 25.93 (5.7 × 10-14 × b-b) | ||
22,048.56 | 10.26 (9.2 × 10-17 × b-b) |
Notes. They correspond to fits performed on the data extracted from the analysis of Porter et al. (2008) and averaged over cylinders of radius and half-height of 2 kpc (model M1) and 0.5 kpc (model M2) about the Earth. We choose M1 as our default ISRF model. In the last column, (a × b-b) indicates that the component can be obtained from a standard black-body spectrum renormalized by a factor of a.
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