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Ultraviolet

The ultraviolet data were taken by IUE on 1994 July 23-24 (i.e. three days prior to the ASCA observation described below.) Due to excessive scattered solar light, we present only the data taken with the short wavelength primary (SWP) camera. These short-wavelength data were taken during one full shift on 1994 July 24 (effective exposure time 8 hours). Data reduction was performed using the ARK software package.

  figure181
Figure 3: IUE (SWP) data for MCG-6-30-15. Note the weak continuum and the prominent CIV tex2html_wrap_inline1432 line.

The resulting SWP spectrum is shown in Fig. 3. The source is found to be weak in the UV compared with other wavebands (apart from radio). The hypothesis that this UV spectrum is flat and featureless can be rejected with a high level of confidence: such a hypothesis gives tex2html_wrap_inline1768 for 65 degrees of freedom (dof). The most significant deviation from the constant model is clearly the CIV tex2html_wrap_inline1432 resonance emission line doublet. Modeling this with a Gaussian profile leads to a highly significant improvements in the goodness of fit ( tex2html_wrap_inline1772 for 3 additional dof). The inferred properties of this line are reported in Table 1. The CIV tex2html_wrap_inline1432 line appears to be significantly broader than the H tex2html_wrap_inline1520 line, and has a FWHM comparable with the `very-broad' component of the H tex2html_wrap_inline1456 line. The CIV line is also blueshifted by tex2html_wrap_inline1780 with respect to the broad Balmer lines. This appears to be a generic feature of high-ionization lines from AGN (e.g. see Espey et al. 1989). This has been interpreted by some authors as evidence for a two-component BLR (e.g. Collin-Souffrin et al. 1988).

There may also be an absorption trough to the blueside of the CIV tex2html_wrap_inline1432 lines. Modeling this with a Gaussian profile leads to a further improvement in the goodness of fit by tex2html_wrap_inline1784 for 3 additional dof. According to the F-test, this is not a significant improvement at the 90 per cent level. Thus, we cannot conclusively determine the reality of this feature and shall not discuss it further.

Formally, the best fit continuum level is tex2html_wrap_inline1786 . It is possible that much of this UV continuum could be stellar in origin. Thus, this value should be considered only as an upper limit to the UV continuum flux from the AGN. High-resolution UV imaging with HST will allow the stellar UV flux to be almost completely separated from the AGN UV flux, thereby allowing these two components to be separated. At the time of writing, such UV imaging has yet to be performed.


next up previous
Next: Other wavebands Up: The Data and basic Previous: The nuclear spectrum

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