Energy Flux Density to Count Rate Conversion Factors (ECF)The following graphs and tables are to be used for proposal planning. They should be used with caution for data analysis. Using the appropriate graph, the HRC (S or I) count rate can be estimated from the incident (unabsorbed) X-ray energy flux density Fx,unab. Four source spectral models have been used: power law, blackbody, thermal bremmstrahlung, and Raymond-Smith (from XSPEC, v10.0) thermal spectrum. For HRC-S, only the central "T" region of the detector is considered here. The energy interval used to calculate the energy flux densities and rates were 0.07 - 10.0 keV. The unabsorbed energy flux density is that energy flux density which would measured at the telescope aperture if there were no interstellar material present (0 hydrogen column density). It is used when the source luminosity Lx and distance R are known. Fx,unab = Lx/4piR2 The count rate CR is given by CR = Fx,unab x ECF ECF is given by
The HRC effective area is given by The ECF graphs and tables are normalized to an incident flux density of 10-10 erg cm2 s-1. |
Detector | Spectrum | Graph (gif) | Graph (ps) | Table | Columns (1-10) |
HRC-S | Power Law | ecf_S_pl.gif | ecf_S_pl.ps | ecf_S_pl.prn | * |
HRC-S | Blackbody | ecf_S_BB.gif | ecf_S_BB.ps | ecf_S_BB.prn | ** |
HRC-S | Bremsstrahlung | ecf_S_BS.gif | ecf_S_BS.ps | ecf_S_BS.prn | ** |
HRC-S | Raymond-Smith | ecf_S_RS.gif | ecf_S_RS.ps | ecf_S_RS.prn | ** |
HRC-I | Power Law | ecf_I_pl.gif | ecf_I_pl.ps | ecf_I_pl.prn | * |
HRC-I | Blackbody | ecf_I_BB.gif | ecf_I_BB.ps | ecf_I_BB.prn | ** |
HRC-I | Bremsstrahlung | ecf_I_BS.gif | ecf_I_BS.ps | ecf_I_BS.prn | ** |
HRC-I | Raymond-Smith | ecf_I_RS.gif | ecf_I_RS.ps | ecf_I_RS.prn | ** |
** kT(keV), NH = 1x1019, 3x1019,1x1020, 3x1020,1x1021, 3x1021,1x1022, 3x1022,1x1023
Ref: Internal memorandum describing calculations. (PDF document)