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122 Chapter 6: Calibration Using Synthetic Photometry Once U(λ) is determined, the absolute flux distribution of any observed source can be computed by simply multiplying the source’s count rate spectrum, C(λ)/∆ t, by U(λ): 2 f λ ( λ ) = U ( λ ) ⋅ C ( λ )/ ∆t (ergs/sec/cm /Å) Synthetic photometry permits a precise generalization of this procedure from the narrow passbands of spectrophotometric pixels to a passband P(λ) of arbitrary width and shape. For a broadband photometric mode the analogous expression giving the detected count rate through passband P is: A C(P) ------------- = ------ ∫ P ( λ ) f λ ( λ )λ dλ hc ∆t The precise definition of mean flux density in a broad passband must then be: P ( λ ) f λ ( λ )λ dλ f λ ( P ) = ∫-----------------------------------------∫ P ( λ )λ dλ so the count rate to flux density conversion factor for a broad passband is: f λ(P) hc / A U λ ( P ) = ---------------------= --------------------------C ( P ) ⁄ ∆t ∫ P ( λ )λ dλ The calibration procedure for broadband photometry is now essentially parallel to that for spectrophotometry. The only difference is that in the spectrophotometric case the source’s flux distribution can be considered constant across the narrow bandwidth of each spectroscopic pixel, whereas in the photometric case the integral over wavelength must be performed more carefully. So the normal method of calibrating photometric modes is to first calculate the mean flux densities of spectrophotometric standard stars in the broad bands, using the known flux spectra and passband shapes, and then derive the flux conversion factors U(P) by comparing the mean flux densities against the corresponding observed count rates. Notice, however, that the last equation above shows us that, if we know the passband function P(λ), we can derive U(P) directly, without the need for standard star observations. This is the technique used by synphot (and incorporated into the WFPC and FOC calibration pipelines) to calibrate HST observing modes. The value of the PHOTFLAM header keyword that appears in calibrated WFPC and FOC images is the flux conversion factor