The zero magnitude of a given ISOPHOT filter is defined as the signal of the `ideal' (i.e. model) Vega which would have been measured in that filter with an infinitely large aperture.
The ideal spectrum of Vega was derived from a Kurucz model with = 9400 K , log() = 3.900, metal poor, 0.0 kms and no infrared excess due to circumstellar dust, extended to 300 m and absolutely calibrated as described by Cohen et al. 1992, [6], and Walker & Cohen 1992, [55].
The magnitude can be obtained from the PHT auto analysis data product by applying the relation:
(D.1) |
where is the AAR flux density. The values for with filter identifier and reference wavelength are listed in Table D.1.
For completeness, we have included in Table D.1 the corresponding powers on the detector , the ideal Vega flux density at the reference wavelength , and the colour correction .
can be applied to the SPD products, thereby taking into account the point spread function correction, see Equations 5.8 and 5.9. The values of are very close to the ones which have been derived for a 10000 K blackbody, see Table C.2.
filter | |||||
ID | [m] | [W] | [Jy] | [Jy] | [ ] |
P_3.29 | 3.3 | 4.60E13 | 312.0 | 318.2 | 0.981 |
P_3.6 | 3.6 | 2.15E12 | 284.7 | 270.9 | 1.051 |
P_4.85 | 4.8 | 1.24E12 | 163.2 | 152.1 | 1.072 |
P_7.3 | 7.3 | 1.01E12 | 79.96 | 71.09 | 1.125 |
P_7.7 | 7.7 | 1.61E13 | 65.14 | 64.23 | 1.014 |
P_10 | 10 | 1.77E13 | 39.40 | 38.60 | 1.021 |
P_11.3 | 11.3 | 3.94E14 | 29.96 | 30.40 | 0.985 |
P_12.8 | 12.8 | 5.71E13 | 35.47 | 26.97 | 1.315 |
P_16 | 15 | 1.26E13 | 24.21 | 23.79 | 1.018 |
P_11.5 | 12 | 5.46E14 | 17.25 | 17.40 | 0.991 |
P_20 | 20 | 5.17E14 | 9.940 | 9.840 | 1.010 |
P_25 | 25 | 3.47E14 | 8.109 | 6.307 | 1.286 |
P_60 | 60 | 7.29E16 | 1.233 | 1.087 | 1.135 |
P_100 | 100 | 3.55E16 | 0.4068 | 0.3866 | 1.052 |
C_50 | 65 | 5.76E16 | 1.197 | 0.9245 | 1.295 |
C_60 | 60 | 7.60E16 | 1.153 | 1.087 | 1.061 |
C_70 | 80 | 5.22E16 | 0.7489 | 0.6075 | 1.233 |
C_90 | 90 | 8.45E16 | 0.5597 | 0.4787 | 1.169 |
C_100 | 100 | 4.03E16 | 0.4261 | 0.3866 | 1.102 |
C_105 | 105 | 2.25E16 | 0.3683 | 0.3503 | 1.052 |
C_120 | 120 | 1.15E16 | 0.3253 | 0.2672 | 1.217 |
C_135 | 150 | 1.32E16 | 0.1862 | 0.1698 | 1.096 |
C_160 | 170 | 1.60E16 | 0.1587 | 0.1316 | 1.205 |
C_180 | 180 | 6.92E17 | 0.1288 | 0.1172 | 1.099 |
C_200 | 200 | 2.27E17 | 0.0972 | 0.0945 | 1.028 |