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jwst_backgrounds/refdata/thermal_curve_jwst_jrigby_v4.0.csv
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#Title: JWST thermal background spectrum to match backgrounds measured in Cycles 1 and 2 | ||
#, Author: Jane Rigby ([email protected]) | ||
#, Date: 5 June 2024 | ||
#, Version: 4.0 | ||
#, Format: comma separated variables (csv) | ||
#, Distribution: unlimited (STI approval in NASA form 1675B.) | ||
#, Columns: wavelength (micron) and equivalent sky radiance (MJy/SR) | ||
#, | ||
#, GENERATED BY: On-orbit thermal model-v3.ipynb. | ||
#, | ||
#, SUMMARY: This is the self-emission thermal background spectrum for JWST, | ||
#, for use in planning observations. At long wavelengths, self-emission | ||
#, from the observatory dominates over astrophysical backgrounds. | ||
#, | ||
#, VERSION HISTORY: v1.X and v2.X were pre-launch predictions used to | ||
#, plan observations for Cycle 1. v3.0 modifed that model to match | ||
#, thermal backgrounds as measured in commissioning (see Rigby, Lightsey | ||
#, et al. 2023, PASP, 135, 048002). | ||
#, | ||
#, DESCRIPTION: Backgrounds were measured by the MIRI team at STScI, from | ||
#, all MIRI imaging observations taken between July 2022 and May 2024. | ||
#, Only observations with Ecliptic latitude >30 degree and Galactic | ||
#, latitude >30 degree were used. For each broadband filter, the | ||
#, background versus time was plotted, and the data fit with two | ||
#, components: a linear component and a sinusoid with period 1 year and | ||
#, max at perihelion. Since the MIRI backgrounds are slowly rising with | ||
#, time, for conservativism in observation planning for Cycle 4, the fits | ||
#, were extrapolated to perihelion (Jan 2026). This process determined | ||
#, the measured backgrounds for the MIRI imaging filters. | ||
#, | ||
#, Since what is needed for observation planning is a thermal spectrum at | ||
#, all relevant wavelengths, not just at the centers of the MIRI imager | ||
#, filters, a physically-motivated model was fit to these data. As in | ||
#, past versions, this simple model approximates JWST as a small number | ||
#, of components (in this case, 33), each represented by a single | ||
#, blackbody. Detailed ray tracing before launch by Paul Lightsey | ||
#, predicted the effective radiances at 10, 15, 20, 25um micron from | ||
#, approximately twenty different components of JWST. | ||
#, (2019.12.03_MIR_summary.xlsx, dated Dec 3 2019, based on integrated | ||
#, thermal model v5.5u4b_EOL_0R_P52P_SL-LTO., which assumed perihelion, | ||
#, hot pitch, and end of life sunshield performance.) For each | ||
#, component, we computed the temperature and effective area x emissivity | ||
#, of the blackbody that could produce those radiances. See Rigby et | ||
#, al. (2023) for details. One can think of "effective area x emissivity" | ||
#, as how effectively the component scatters thermal emission into the | ||
#, JWST beam. | ||
#, | ||
#, An improvement over previous versions is the treatment of the primary | ||
#, mirror; it is no longer modeled as a single blackbody, but instead is | ||
#, now modeled with one blackbody for each of the 18 primary mirror | ||
#, segments, with segment temperatures measured 1/2024. The PM segments | ||
#, are assumed to have equal effective area x emissivity. | ||
#, | ||
#, As in previous versions, the model approximates JWST with 15 | ||
#, additional blackbodies representing major components. What is new is | ||
#, that measured on-orbit temperatures are now used for components that | ||
#, have thermal sensors. Of these 15 components, 9 have measured | ||
#, temperatures (PM frill, core, DTA tower, ISIM bench, TM FSM mask, AOS | ||
#, bench, secondary mirror, SM support structures,and BSF). The other 6 | ||
#, components do not have any temperature sensors (sunshield, sunshield | ||
#, spreaders, bib, AOS exterior, SS layer 4 leakage, and SS light line | ||
#, tolerance). | ||
#, | ||
#, To fit the operational MIRI imager data, temperatures of components | ||
#, without measured temperatures were adjusted by hand, the frill was set | ||
#, 4K hotter than the measurements, and a small hot source (T~280K) was | ||
#, added to explain the short-wavelength MIRI data, while not | ||
#, over-predicting measurements from NIRCam at 4.4 micron. This is by no | ||
#, means a unique fit, but represents the backgrounds seen in Cycles 1 and 2 | ||
#, better than the current post-commissioning. Work is ongoing to improve | ||
#, the measurement of the JWST thermal background. | ||
# | ||
5.000E-01,0.000E+00 | ||
6.000E-01,0.000E+00 | ||
7.000E-01,0.000E+00 | ||
8.000E-01,0.000E+00 | ||
9.000E-01,0.000E+00 | ||
1.000E+00,0.000E+00 | ||
1.100E+00,0.000E+00 | ||
1.200E+00,0.000E+00 | ||
1.300E+00,0.000E+00 | ||
1.400E+00,0.000E+00 | ||
1.500E+00,1.873E-10 | ||
1.600E+00,1.313E-09 | ||
1.700E+00,7.241E-09 | ||
1.800E+00,3.270E-08 | ||
1.900E+00,1.249E-07 | ||
2.000E+00,4.141E-07 | ||
2.100E+00,1.216E-06 | ||
2.200E+00,3.216E-06 | ||
2.300E+00,7.770E-06 | ||
2.400E+00,1.735E-05 | ||
2.500E+00,3.614E-05 | ||
2.600E+00,7.083E-05 | ||
2.700E+00,1.315E-04 | ||
2.800E+00,2.327E-04 | ||
2.900E+00,3.943E-04 | ||
3.000E+00,6.430E-04 | ||
3.100E+00,1.013E-03 | ||
3.200E+00,1.545E-03 | ||
3.300E+00,2.292E-03 | ||
3.400E+00,3.313E-03 | ||
3.500E+00,4.678E-03 | ||
3.600E+00,6.463E-03 | ||
3.700E+00,8.756E-03 | ||
3.800E+00,1.165E-02 | ||
3.900E+00,1.524E-02 | ||
4.000E+00,1.964E-02 | ||
4.100E+00,2.495E-02 | ||
4.200E+00,3.128E-02 | ||
4.300E+00,3.874E-02 | ||
4.400E+00,4.744E-02 | ||
4.500E+00,5.749E-02 | ||
4.600E+00,6.899E-02 | ||
4.700E+00,8.204E-02 | ||
4.800E+00,9.673E-02 | ||
4.900E+00,1.131E-01 | ||
5.000E+00,1.314E-01 | ||
5.100E+00,1.514E-01 | ||
5.200E+00,1.734E-01 | ||
5.300E+00,1.974E-01 | ||
5.400E+00,2.234E-01 | ||
5.500E+00,2.515E-01 | ||
5.600E+00,2.816E-01 | ||
5.700E+00,3.138E-01 | ||
5.800E+00,3.480E-01 | ||
5.900E+00,3.844E-01 | ||
6.000E+00,4.228E-01 | ||
6.100E+00,4.633E-01 | ||
6.200E+00,5.058E-01 | ||
6.300E+00,5.503E-01 | ||
6.400E+00,5.967E-01 | ||
6.500E+00,6.451E-01 | ||
6.600E+00,6.954E-01 | ||
6.700E+00,7.475E-01 | ||
6.800E+00,8.013E-01 | ||
6.900E+00,8.569E-01 | ||
7.000E+00,9.143E-01 | ||
7.100E+00,9.732E-01 | ||
7.200E+00,1.034E+00 | ||
7.300E+00,1.096E+00 | ||
7.400E+00,1.160E+00 | ||
7.500E+00,1.225E+00 | ||
7.600E+00,1.291E+00 | ||
7.700E+00,1.359E+00 | ||
7.800E+00,1.429E+00 | ||
7.900E+00,1.500E+00 | ||
8.000E+00,1.572E+00 | ||
8.100E+00,1.645E+00 | ||
8.200E+00,1.720E+00 | ||
8.300E+00,1.797E+00 | ||
8.400E+00,1.874E+00 | ||
8.500E+00,1.954E+00 | ||
8.600E+00,2.034E+00 | ||
8.700E+00,2.117E+00 | ||
8.800E+00,2.201E+00 | ||
8.900E+00,2.286E+00 | ||
9.000E+00,2.374E+00 | ||
9.100E+00,2.463E+00 | ||
9.200E+00,2.554E+00 | ||
9.300E+00,2.648E+00 | ||
9.400E+00,2.744E+00 | ||
9.500E+00,2.842E+00 | ||
9.600E+00,2.943E+00 | ||
9.700E+00,3.046E+00 | ||
9.800E+00,3.153E+00 | ||
9.900E+00,3.263E+00 | ||
1.000E+01,3.376E+00 | ||
1.010E+01,3.493E+00 | ||
1.020E+01,3.613E+00 | ||
1.030E+01,3.738E+00 | ||
1.040E+01,3.868E+00 | ||
1.050E+01,4.002E+00 | ||
1.060E+01,4.142E+00 | ||
1.070E+01,4.287E+00 | ||
1.080E+01,4.438E+00 | ||
1.090E+01,4.595E+00 | ||
1.100E+01,4.758E+00 | ||
1.110E+01,4.929E+00 | ||
1.120E+01,5.107E+00 | ||
1.130E+01,5.293E+00 | ||
1.140E+01,5.488E+00 | ||
1.150E+01,5.691E+00 | ||
1.160E+01,5.904E+00 | ||
1.170E+01,6.126E+00 | ||
1.180E+01,6.359E+00 | ||
1.190E+01,6.603E+00 | ||
1.200E+01,6.858E+00 | ||
1.210E+01,7.125E+00 | ||
1.220E+01,7.405E+00 | ||
1.230E+01,7.699E+00 | ||
1.240E+01,8.006E+00 | ||
1.250E+01,8.328E+00 | ||
1.260E+01,8.665E+00 | ||
1.270E+01,9.018E+00 | ||
1.280E+01,9.387E+00 | ||
1.290E+01,9.774E+00 | ||
1.300E+01,1.018E+01 | ||
1.310E+01,1.060E+01 | ||
1.320E+01,1.105E+01 | ||
1.330E+01,1.151E+01 | ||
1.340E+01,1.200E+01 | ||
1.350E+01,1.251E+01 | ||
1.360E+01,1.304E+01 | ||
1.370E+01,1.359E+01 | ||
1.380E+01,1.417E+01 | ||
1.390E+01,1.478E+01 | ||
1.400E+01,1.541E+01 | ||
1.410E+01,1.607E+01 | ||
1.420E+01,1.676E+01 | ||
1.430E+01,1.748E+01 | ||
1.440E+01,1.823E+01 | ||
1.450E+01,1.902E+01 | ||
1.460E+01,1.983E+01 | ||
1.470E+01,2.068E+01 | ||
1.480E+01,2.157E+01 | ||
1.490E+01,2.250E+01 | ||
1.500E+01,2.346E+01 | ||
1.510E+01,2.447E+01 | ||
1.520E+01,2.551E+01 | ||
1.530E+01,2.660E+01 | ||
1.540E+01,2.773E+01 | ||
1.550E+01,2.891E+01 | ||
1.560E+01,3.014E+01 | ||
1.570E+01,3.141E+01 | ||
1.580E+01,3.274E+01 | ||
1.590E+01,3.412E+01 | ||
1.600E+01,3.555E+01 | ||
1.610E+01,3.704E+01 | ||
1.620E+01,3.859E+01 | ||
1.630E+01,4.020E+01 | ||
1.640E+01,4.187E+01 | ||
1.650E+01,4.361E+01 | ||
1.660E+01,4.541E+01 | ||
1.670E+01,4.729E+01 | ||
1.680E+01,4.923E+01 | ||
1.690E+01,5.125E+01 | ||
1.700E+01,5.334E+01 | ||
1.710E+01,5.552E+01 | ||
1.720E+01,5.777E+01 | ||
1.730E+01,6.011E+01 | ||
1.740E+01,6.254E+01 | ||
1.750E+01,6.505E+01 | ||
1.760E+01,6.766E+01 | ||
1.770E+01,7.036E+01 | ||
1.780E+01,7.317E+01 | ||
1.790E+01,7.607E+01 | ||
1.800E+01,7.908E+01 | ||
1.810E+01,8.220E+01 | ||
1.820E+01,8.543E+01 | ||
1.830E+01,8.878E+01 | ||
1.840E+01,9.224E+01 | ||
1.850E+01,9.583E+01 | ||
1.860E+01,9.955E+01 | ||
1.870E+01,1.034E+02 | ||
1.880E+01,1.074E+02 | ||
1.890E+01,1.115E+02 | ||
1.900E+01,1.158E+02 | ||
1.910E+01,1.202E+02 | ||
1.920E+01,1.247E+02 | ||
1.930E+01,1.294E+02 | ||
1.940E+01,1.343E+02 | ||
1.950E+01,1.394E+02 | ||
1.960E+01,1.446E+02 | ||
1.970E+01,1.499E+02 | ||
1.980E+01,1.555E+02 | ||
1.990E+01,1.613E+02 | ||
2.000E+01,1.672E+02 | ||
2.010E+01,1.733E+02 | ||
2.020E+01,1.797E+02 | ||
2.030E+01,1.862E+02 | ||
2.040E+01,1.929E+02 | ||
2.050E+01,1.999E+02 | ||
2.060E+01,2.071E+02 | ||
2.070E+01,2.145E+02 | ||
2.080E+01,2.221E+02 | ||
2.090E+01,2.300E+02 | ||
2.100E+01,2.381E+02 | ||
2.110E+01,2.465E+02 | ||
2.120E+01,2.551E+02 | ||
2.130E+01,2.640E+02 | ||
2.140E+01,2.732E+02 | ||
2.150E+01,2.826E+02 | ||
2.160E+01,2.923E+02 | ||
2.170E+01,3.023E+02 | ||
2.180E+01,3.126E+02 | ||
2.190E+01,3.232E+02 | ||
2.200E+01,3.341E+02 | ||
2.210E+01,3.454E+02 | ||
2.220E+01,3.569E+02 | ||
2.230E+01,3.688E+02 | ||
2.240E+01,3.810E+02 | ||
2.250E+01,3.935E+02 | ||
2.260E+01,4.064E+02 | ||
2.270E+01,4.197E+02 | ||
2.280E+01,4.333E+02 | ||
2.290E+01,4.472E+02 | ||
2.300E+01,4.616E+02 | ||
2.310E+01,4.763E+02 | ||
2.320E+01,4.915E+02 | ||
2.330E+01,5.070E+02 | ||
2.340E+01,5.230E+02 | ||
2.350E+01,5.393E+02 | ||
2.360E+01,5.561E+02 | ||
2.370E+01,5.733E+02 | ||
2.380E+01,5.909E+02 | ||
2.390E+01,6.090E+02 | ||
2.400E+01,6.276E+02 | ||
2.410E+01,6.466E+02 | ||
2.420E+01,6.660E+02 | ||
2.430E+01,6.860E+02 | ||
2.440E+01,7.064E+02 | ||
2.450E+01,7.273E+02 | ||
2.460E+01,7.487E+02 | ||
2.470E+01,7.706E+02 | ||
2.480E+01,7.931E+02 | ||
2.490E+01,8.160E+02 | ||
2.500E+01,8.395E+02 | ||
2.510E+01,8.635E+02 | ||
2.520E+01,8.881E+02 | ||
2.530E+01,9.132E+02 | ||
2.540E+01,9.389E+02 | ||
2.550E+01,9.651E+02 | ||
2.560E+01,9.920E+02 | ||
2.570E+01,1.019E+03 | ||
2.580E+01,1.047E+03 | ||
2.590E+01,1.076E+03 | ||
2.600E+01,1.105E+03 | ||
2.610E+01,1.135E+03 | ||
2.620E+01,1.165E+03 | ||
2.630E+01,1.197E+03 | ||
2.640E+01,1.228E+03 | ||
2.650E+01,1.261E+03 | ||
2.660E+01,1.294E+03 | ||
2.670E+01,1.327E+03 | ||
2.680E+01,1.362E+03 | ||
2.690E+01,1.397E+03 | ||
2.700E+01,1.432E+03 | ||
2.710E+01,1.469E+03 | ||
2.720E+01,1.506E+03 | ||
2.730E+01,1.544E+03 | ||
2.740E+01,1.582E+03 | ||
2.750E+01,1.622E+03 | ||
2.760E+01,1.662E+03 | ||
2.770E+01,1.702E+03 | ||
2.780E+01,1.744E+03 | ||
2.790E+01,1.786E+03 | ||
2.800E+01,1.829E+03 | ||
2.810E+01,1.873E+03 | ||
2.820E+01,1.917E+03 | ||
2.830E+01,1.963E+03 | ||
2.840E+01,2.009E+03 | ||
2.850E+01,2.056E+03 | ||
2.860E+01,2.103E+03 | ||
2.870E+01,2.152E+03 | ||
2.880E+01,2.201E+03 | ||
2.890E+01,2.251E+03 | ||
2.900E+01,2.302E+03 | ||
2.910E+01,2.354E+03 | ||
2.920E+01,2.407E+03 | ||
2.930E+01,2.461E+03 | ||
2.940E+01,2.515E+03 | ||
2.950E+01,2.570E+03 | ||
2.960E+01,2.626E+03 | ||
2.970E+01,2.683E+03 | ||
2.980E+01,2.741E+03 | ||
2.990E+01,2.800E+03 | ||
3.000E+01,2.860E+03 | ||
3.010E+01,2.920E+03 | ||
3.020E+01,2.982E+03 | ||
3.030E+01,3.044E+03 | ||
3.040E+01,3.107E+03 | ||
3.050E+01,3.172E+03 | ||
3.060E+01,3.237E+03 | ||
3.070E+01,3.303E+03 | ||
3.080E+01,3.370E+03 | ||
3.090E+01,3.438E+03 | ||
3.100E+01,3.507E+03 |