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Extinction of the continuum source

The optical continuum radiation will also be affected by extinction and reddening. Suppose the intrinsic spectrum of the (optical) continuum has a form tex2html_wrap_inline1988 . Furthermore, suppose that the observed (i.e. reddened) optical continuum spectrum is tex2html_wrap_inline1990 . The difference between tex2html_wrap_inline1520 and tex2html_wrap_inline1994 is related to the reddening towards the source. From the definition of reddening, it is easily seen that

eqnarray267

where tex2html_wrap_inline1996 and tex2html_wrap_inline1998 are the frequencies characterizing the B-band and V-band respectively.

Unreddened Seyfert 1 nuclei in the luminosity range occupied by MCG-6-30-15 tend to have optical continua with tex2html_wrap_inline2006 (e.g. see study of Morris & Ward 1988, and note that a flat flux spectrum in wavelength space implies tex2html_wrap_inline2008 when considered in frequency space). Fitting the (galaxy-subtracted) blue spectrum of the nucleus of MCG-6-30-15, we conclude that tex2html_wrap_inline1994 lies in the range 4.5-5. Assuming that the intrinsic optical spectrum of MCG-6-30-15 is similar to that found in unreddened Seyfert 1 nuclei, the reddening of the optical continuum source E(B-V) is in the range 0.65-0.78.

The reddening of the optical continuum source is consistent with the lower end of the reddening derived from the H tex2html_wrap_inline1520 /H tex2html_wrap_inline1456 Balmer ratio. Assuming that the optical continuum is associated with an accretion disk embedded inside the BLR, this result suggests that little dust is present between the accretion disk and the region where the bulk of the the broad line photons are emitted.



Chris Reynolds
Wed Jul 2 14:33:32 MDT 1997