Next Contents Previous


The ionizing continuum shape in AGN is difficult to study directly. At low redshift it is mostly obscured by our own interstellar medium, and inferences must be made from the spectral shape observed in the far-UV and soft X-ray (on either side of the opaque interstellar absorption) as well as from clues provided by the emission lines observed. The notion that continuum radiation of AGN peaked in the unobservable extreme ultraviolet can be traced back to the accretion-disk fits of Malkan & Sargent (1982) as well as the "big blue bump" suggested by the UV and soft X-ray excesses of PG1211+143 (Bechtold et al. 1987). Accounting for the fluxes in the broad emission lines led Mathews & Ferland (1987) to adopt an ionizing spectral shape peaking in the extreme ultraviolet (see Fig. 2).

Figure 2

Figure 2. Schematic representations of inferred spectral energy distributions of AGN after Laor et al. (1997). The nu-0.3 e-hnu / kT curve approximates a simple accretion disk spectrum.

More recent work that uses ensembles of objects to produce a "composite" spectrum over the observable wavelength range suggests that there is no extreme ultraviolet peak. The UV composites of Zheng et al. (1997) for radio-loud (RL) and radio-quiet (RQ) objects, shown schematically in Fig. 2, have a blue far-UV continuum with a distinct break to a steeper spectral index (fnu ~ nu-1.8) at ~ 1000 Å. Soft X-ray spectral composites constructed by Laor et al. (1997) have slopes similar to the short wavelength end of the UV composites.

The Zheng et al. (1997) composite builds upon the earlier examples of Baldwin (1977) and Francis et al. (1991) to produce an average QSO spectrum from HST ultraviolet spectra of 100 different QSOs. This composite consists of all FOS observations of QSOs with z > 0.33 prior to 1996 January 1. To construct the composite, the observed fluxes were first corrected for foreground Galactic reddening with a Seaton (1979) law using extinction as specified by Burstein & Heiles (1978). Strong Lyman alpha lines and visible Lyman-limit systems were corrected in the individual spectra. (Objects with strong intrinsic absorption such as BALQSOs were simply omitted from the composite.) Fainter Lyalpha forest lines and the "Lyman valley" (Møller & Jakobsen 1990) were corrected for statistically as a function of redshift. The result from Zheng et al. (1997) is shown in Fig. 3.

Figure 3

Figure 3. The composite QSO spectrum of Zheng et al. (1997) shows a break in spectral index at 1000 Å where it flattens to fnu ~ nu-1.7. An updated composite using more than two times as many quasars (Telfer et al. 2000) shows the same characteristics. The far-UV spectrum of 3C 273 is qualitatively similar to both - the spectrum breaks at 1030 Å to an index of 1.7 ± 0.36.

Work currently in progress by Telfer et al. (2000) is updating this composite spectrum using the same technique with a sample that is nearly three times larger. Containing spectra of 248 QSOs obtained prior to 2000 May 31, the Telfer et al. (2000) composite is nearly identical to the Zheng et al. (1997) result. A physical interpretation of the spectral shape observed by Zheng et al. (1997) is that the typical AGN spectrum is Comptonized radiation from an accretion disk. A spectral break near the Lyman limit is a characteristic expected in Comptonized accretion-disk spectra. Comptonization smears out the Lyman-limit edge of the intrinsic accretion-disk spectrum and produces a power-law tail at wavelengths shortward of ~ 1000 Å. Although a simple model of a Comptonized disk provides a good fit to the Zheng et al. composite, there is the nagging question of how physical such a composite is, and whether its shape holds any physical meaning since the individual spectra of the sample QSOs vary in shape over quite a wide range. The study of the 3C 273 far-UV spectrum by Kriss et al. (1999) provides a firm physical basis for the interpretation of the Zheng et al. composite. In the 3C 273 spectrum (also shown in Fig. 3), one sees the same qualitative characteristics as in the composite spectrum - the spectral index steepens at ~ 1000 Å in the rest frame. As shown further in Fig. 4, the shorter-wavelength UV spectrum extrapolates very well to the observed soft-X-ray spectrum. Both the composite spectra and the spectrum of 3C 273 leave little room in the extreme ultraviolet for a big bump in the QSO spectral energy distribution.

Figure 4

Figure 4. The far-UV and soft X-ray spectra of 3C 273 allow little room for a bump in the extreme ultraviolet.

The apparent lack of an extreme ultraviolet peak in the ionizing spectrum now leaves us in a quandary. The analysis of Mathews & Ferland (1987) based on the broad emission line fluxes is still valid; Korista, Ferland, & Baldwin (1997) suggest that the BLR "sees" a different continuum shape than we do since the He II lambda1640 equivalent widths in moderate redshift QSOs require more ionizing photons than are present in the Zheng et al. composite. On the other hand, the mean spectral index of the QSO composite matches the ionization requirements for H I and He II absorption by the IGM (Zhang et al. 1997), so apparently the IGM is seeing the same average that we are. It may be that the answer lies in detailed studies of individual objects. Objects with high He II equivalent widths may dominate the He II average, but these same objects may not be represented in the sample of spectra contributing to the composite at short wavelengths. Far-UV and soft X-ray spectra of objects at moderate redshift that tightly constrain the possible EUV spectral shape (as shown above for 3C 273) may resolve this issue.

Next Contents Previous