The Ages of Quasar Host Galaxies
Total Page:16
File Type:pdf, Size:1020Kb
Mon. Not. R. Astron. Soc. 000, 000–000 (0000) Printed 30 October 2018 (MN LATEX style file v1.4) The ages of quasar host galaxies. L.A. Nolan1, J.S. Dunlop1, M.J. Kukula1, D. H. Hughes1,2, T. Boroson3 & R. Jimenez1. 1Institute for Astronomy, University of Edinburgh, Blackford Hill, Edinburgh, EH9 3HJ 2INOAE, Apartado Postal 51 y 216, 72000, Puebla, Pue., Mexico. 3NOAO, PO Box 26732, Tucson, Arizona 85726−6732, U.S.A. Submitted for publication in MNRAS ABSTRACT We present the results of fitting deep off-nuclear optical spectra of radio-quiet quasars, radio-loud quasars and radio galaxies at z ≃ 0.2 with evolutionary synthesis models of galaxy evolution. Our aim was to determine the age of the dynamically dominant stellar populations in the host galaxies of these three classes of powerful AGN. Some of our spectra display residual nuclear contamination at the shortest wavelengths, but the detailed quality of the fits longward of the 4000A˚ break provide unequivocal proof, if further proof were needed, that quasars lie in massive galaxies with (at least at z ≃ 0.2) evolved stellar populations. By fitting a two-component model we have separated the very blue (starburst and/or AGN contamination) from the redder underlying spectral energy distribution, and find that the hosts of all three classes of AGN are dominated by old stars of age 8 − 14 Gyr. If the blue component is attributed to young stars, we find that, at most, 1% of the visible baryonic mass of these galaxies is involved in star-formation activity at the epoch of observation, at least over the region sampled by our spectroscopic observations. These results strongly arXiv:astro-ph/0002020v2 23 Oct 2000 support the conclusion reached by McLure et al. (1999) that the host galaxies of luminous quasars are massive ellipticals which have formed by the epoch of peak quasar activity at z ≃ 2.5. Key words: galaxies: active – galaxies: evolution – galaxies: stellar content – quasars: general 1 INTRODUCTION tive glaxies (Maggorian et al. 1998) has further strengthened the motivation for exploring the link between active AGN Determining the nature of the host galaxies of powerful ac- and the dynamical and spectral properties of their hosts. tive galactic nuclei (AGN) is of importance not only for Over the last few years, improvements in imaging res- improving our understanding of different manifestations of olution offered by both space-based and ground-based op- AGN activity, but also for exploring possible relationships tical/infrared telescopes has stimulated a great deal of re- between nuclear activity and the evolution of massive galax- search activity aimed at determining the basic structural ies. The recent affirmation that black-hole mass appears ap- parameters (i.e. luminosity, size and morphological type) proximately proportional to spheroid mass in nearby inac- of the hosts of radio-loud quasars, radio-quiet quasars, and c 0000 RAS 2 L.A. Nolan et al. lower-luminosity X-ray-selected and optically-selected AGN activity refer to the region probed by our observations ≃ 5 (e.g. Disney et al. 1995; Hutchings & Morris 1995; Bahcall arcsec off-nucleus. However, given the large scalelengths of et al. 1997; Hooper et al. 1997; McLure et al. 1999, Schade et the hosts, their relatively modest redshift, and the fact that al. 2000). However, relatively little corresponding effort has our spectra are derived from long-slit observations, it is rea- been invested in spectroscopic investigations of AGN hosts, sonable to regard our conclusions as applying to fairly typ- despite the fact that this offers an independent way of clas- ical regions, still located well within the bulk of the host sifying these galaxies, as well as a means of estimating the galaxies under investigation. age of their stellar populations. The layout of this paper is as follows. In section 2 we Our own work in this field to date has focussed on provide details of the adopted models, and how they have the investigation of the hosts of matched samples of radio- been fitted to the data. The results are presented in section quiet quasars (RQQs), radio-loud quasars (RLQs) and radio 3, along with detailed notes on the fitting of individual spec- galaxies (RGs) at relatively modest redshift (z = 0.2). De- tra. The implications of the model fits are then discussed tails of these samples can be found in Dunlop et al. (1993). in section 4, focussing on a comparison of the typical de- In brief, the sub-samples of quasars (i.e. RQQs and RLQs) rived host-galaxy ages in the three AGN subsamples. Finally have been selected to be indistinguishable in terms of their our conclusions are summarized in section 5. The detailed two-dimensional distribution on the V − z plane, while the model fits, along with corresponding chi-squared plots are sub-samples of radio-loud AGN (i.e. RLQs and RGs) have presented in Appendix A. been selected to be indistinguishable in terms of their two- dimensional distribution on the P5GHz − z plane (as well as having indistinguishable spectral-index distributions). Deep 2 SPECTRAL FITTING. infrared imaging of these samples (Dunlop et al. 1993; Tay- lor et al. 1996) has recently been complemented by deep The stellar population synthesis models adopted for age- WFPC2 HST optical imaging (McLure et al. 1999), the fi- dating the AGN host galaxy stellar populations are the so- nal results of which are reported by Dunlop et al. (2000). lar metallicity, instantaneous starburst models of Jimenez As well as demonstrating that, dynamically, the hosts of et al. (2000). We have endeavoured to fit each off-nuclear all three types of luminous AGN appear indistinguishable host galaxy optical spectrum by a combination of two sin- from normal ellipticals, this work has enabled us to deduce gle starburst components. For the first component, age is crude spectral information on the host galaxies in the form fitted as a free parameter, while for the second component of optical-infrared colours. However, broad-baseline colour the age is fixed at 0.1 Gyr, and the normalization relative to information can clearly be most powerfully exploited if com- the first component is the only free parameter. This dual- bined with detailed optical spectroscopy. Over the past few component approach was adopted because single-age models years we have therefore attempted to complement our imag- are not able to adequately represent the data, and because ing studies with a programme of deep optical off-nuclear it allows the age of the dynamically dominant component to spectroscopy of this same sample of AGN. be determined in a way which is not overly reliant on the Details of the observed samples, spectroscopic obser- level of ultraviolet flux which might be contributed either vations, and the basic properties of the observed off-nuclear by a recent burst of star-formation, or by contamination of spectra are given in a companion paper (Hughes et al. 2000). the slit by scattered light from the quasar nucleus. After ex- As discussed by Hughes et al. (2000), the key feature of this perimentation it was found that the spectral shape of the study (other than its size, depth, and sample control) is that blue light was better represented by the 0.1 Gyr-old (solar we have endeavoured to obtain spectra from positions fur- metallicity) model of Jimenez than by models of greater (in- ther off-nucleus (≃ 5 arcsec) than previous workers, in an termediate) age (e.g. 1 Gyr). Moreover, the further addition attempt to better minimize the need for accurate subtrac- of a third intermediate age component, ≃ 1 Gyr, did not tion of contaminating nuclear light. This approach was made significantly improve the quality of the fits achieved. possible by our deep infrared imaging data, which allowed In general, our data are of insufficient quality to tell us to select slit positions ≃ 5 arcsec off-nucleus which still whether the component which dominates at λ ≃ 3000A˚ re- intercepted the brighter isophotes of the host galaxies (slit ally is due to young stars, or is produced by direct or scat- positions are shown, superimposed on the infrared images, tered quasar light. However, while the origin of the blue light in Hughes et al. 2000). is obviously of some interest, it has little impact on the main In this paper we present the results of attempting to fit results presented in this paper, which refer to the age of the the resulting off-nuclear spectra with evolutionary synthesis dynamically dominant stellar population which dominates models of galaxy evolution. Our primary aim was to de- the spectrum from longward of the 4000A˚ break through to termine whether, in each host galaxy, the optical spectrum the near infrared. The robustness of the age determination could be explained by the same model as the optical-infrared of the dominant population is demonstrated by comparing colour, and, if so, to derive an estimate of the age of the dy- the results of the two stellar-population model fit with the namically dominant stellar population. However, this study results of a fit allowi ng for a nuclear contribution as well as also offered the prospect of determining whether the hosts of the two stellar populations. different classes of AGN differ in terms of their more recent The model parameters determined were therefore the star-formation activity. age of the dominant stellar population, which we can reason- It is worth noting that our off-nuclear spectroscopy ob- ably call the age of the galaxy, and the fraction, by (visible) viously does not enable us to say anything about the level of baryonic mass, of the 0.1 Gyr component.