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2001, Monthly Notices of the Royal Astronomical Society
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 active galactic nuclei (AGN). Some of our spectra display residual nuclear contamination at the shortest wavelengths, but the detailed quality of the fits longward of the 4000-A Ê break provides 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 per cent 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 support the conclusion reached by McLure et al. that the host galaxies of luminous quasars are massive ellipticals which have formed by the epoch of peak quasar activity at z .
The Astrophysical Journal, 2007
We use the spectra of ≈22,000 nearby early-type galaxies from the Sloan Digital Sky Survey (SDSS) to determine the age distribution of these galaxies as a function of their velocity dispersion σ v in the range 100 km s −1 ∼ < σ v ∼ < 280 km s −1 . We then combine the inferred age-distributions with the local abundance of spheroids, including early-type galaxies and late-type bulges, to predict the evolution of the quasar luminosity function (LF) in the redshift range 0 < z ∼ < 6. We make the following simple assumptions: (i) the formation of stars in each galaxy, at the epoch identified with the mean mass-weighted stellar age, is accompanied by the prompt assembly of the nuclear supermassive black hole (SMBH); (ii) the mass of the SMBH obeys the M bh − σ v correlation observed in nearby galaxies; (iii) the SMBH radiates at a fraction f Edd of the Eddington limit for a fixed duration t Q , and is identified as a luminous quasar during this epoch, (iv) the intrinsic dispersions in the Eddington ratio and the M bh − σ v relation produce a combined scatter of ∆ log L Q around the mean logarithmic quasar luminosity log L Q at fixed σ v . These assumptions require that the SMBH remnants of quasars with L bol ∼ < 10 12.5 f Edd L ⊙ reside predominantly in bulges of late type galaxies. We find that evolution of the observed quasar LF can be fit over the entire redshift range in this simple model, 0 < z ∼ < 6 with the choices of 0.6 ∼ < ∆ log L Q ∼ < 0.9, 6 × 10 7 yr ∼ < t Q ∼ < 8 × 10 7 yr, and 0.3 ∼ < f Edd ∼ < 0.5. We find no evidence that any of the model parameters evolves with redshift, supporting the strong connection between the formation of stars and nuclear SMBHs in spheroids.
The Astrophysical Journal, 2004
We present the results of a near-infrared imaging study of the host galaxies of 17 quasars in the redshift range 1< z <2. The observations were carried out at the ESO VLT UT1 8m telescope under excellent seeing conditions (∼ 0. ′′ 4). The sample includes radio-loud (RLQ) and radio-quiet (RQQ) quasars with similar distribution of redshift and optical luminosity. For all the observed objects but one we have been able to derive the global properties of the surrounding nebulosity. The host galaxies of both types of quasars appear to follow the expected trend in luminosity of massive ellipticals undergoing simple passive evolution. However, * * *
Astron J, 2001
Deep optical images have been gathered for a nearly complete sample of radio galaxies from the Revised 3rd Cambridge (3CR) Catalog in the redshift range 0.15 < z < 0.65. Total and nuclear magnitudes and colors have been extracted. The richness of the galaxy clustering environment has also been quantified by calculating the amplitude of the galaxy-galaxy spatial covariance function (B gg), showing overdensities ranging up to Abell class 0-1 clusters. These optical data are compared to similar data from an existing sample of radio-loud quasars in the same redshift range for the purpose of determining the relationship between radio galaxies and quasars. In the range 0.15 < z < 0.4, we find that quasars and radio galaxies have significantly different environments in that only radio galaxies are found in rich cluster environments. This comparison appears to rule out the hypothesis that all quasars are radio galaxies viewed from a particular angle at the 97% confidence level (99.6% confidence level if N-galaxies are considered quasars). The existence of quasars in clusters at z > 0.4 supports the hypothesis that some radio-loud quasars may dim with time and evolve into radio galaxies with an efolding time of ∼ 0.9 Gyr. A compatible scenario is presented for this evolution in which the quasar dims due to the absence of low velocity interactions between the quasar host and companion galaxies which trigger quasar activity and/or a diminishing fuel supply caused by the more effective gas "sweeping" of a growing intracluster medium.
Monthly Notices of the Royal Astronomical Society, 2010
There is increasing evidence of a connection between AGN activity and galaxy evolution. To obtain further insight into this potentially important evolutionary phase, we analyse the properties of quasar host galaxies. In this paper, we present a population synthesis modeling technique for off-axis spectra, the results of which constrain host colour and the stellar ages of luminous quasars (M V (nuc) < −23). Our technique is similar to well established quiescent-galaxy models, modified to accommodate scattered nuclear light (a combination of atmospheric, instrumental and host galaxy scattered light) observed off axis. In our model, subtraction of residual scattered quasar light is performed, while simultaneously modeling the constituent stellar populations of the host galaxy. The reliability of this technique is tested via a Monte-Carlo routine in which the correspondence between synthetic spectra with known parameters and the model output is determined. Application of this model to a preliminary sample of 10 objects is presented and compared to previous studies. Spectroscopic data was obtained via long-slit and integral-field unit observations on the Keck and WIYN telescopes. We confirm that elliptical quasar hosts are distinguishable (bluer) from inactive ellipticals in rest frame B-V colour. Additionally, we note a trend for radio luminous (L 5GHz 10 40 erg s −1 ) quasars to be located in redder host galaxies in comparison to their less luminous radio counterparts. While the host colour and age of our radio luminous sample is in close proximity to the green valley, our radio faint sample is consistent with quiescent star-forming galaxies. However, further observations are needed to confirm these results. Finally, we discuss future applications for our technique on a larger sample of objects being obtained via SALT and WIYN telescope observing campaigns.
Monthly Notices of the Royal Astronomical Society, 1999
We compare the evolution with cosmic time of the star formation rate per comoving volume in galaxies and of the volume emissivity due to active galactic nuclei, in an attempt to understand the relationship between black hole accretion and the formation of the surrounding structure. We find an interesting similarity between the evolution rates for the total populations of galaxies and AGN, which indicates that, on average, the history of black hole accretion follows that of stellar formation in the host galaxies. Similarly, the evolution of luminous quasars parallels that of the stellar populations in massive spheroidal galaxies, in keeping with the locally established association of supermassive black holes and galactic bulges. We finally comment on our finding that high-luminosity, high-mass systems evolve on a shorter cosmic timescale than lower mass ones; to explain this, theories of structure formation based on the gravitational collapse of dark matter haloes must be complemented with a detailed description of the dynamical processes in the baryonic component, which dominate the formation and evolution in high-density environments.
Monthly Notices of the Royal Astronomical Society, 2013
We analyse the optical spectra of massive (log M * /M > 11.4) radio-loud galaxies at z ∼ 0.2 and z ∼ 0.6. Our samples are generated by cross-matching the Sloan Digital Sky Survey DR7 and Baryon Oscillation Spectroscopic Survey spectroscopic galaxy catalogues with the Faint Images of the Radio Sky at Twenty centimetres and NVSS radio continuum surveys. By comparing stellar population parameters of these radio-loud samples with radio-quiet control samples matched in stellar mass, velocity dispersion and redshift, we investigate how the presence of a radio-emitting jet relates to the recent star formation history of the host galaxy. We also investigate how the emission-line properties of the radio galaxies evolve with redshift by stacking their spectra. Our main results are the following. (1) Both at low and at high redshift, half as many radio-loud as radio-quiet galaxies have experienced significant star formation in the past Gyr. This difference in star formation history is independent of the luminosity of the radio AGN, except at radio luminosities greater than 10 25.5 W Hz −1 , where it disappears. (2) The Balmer absorption-line properties of massive galaxies that have experienced recent star formation show that star formation occurred as a burst in many of these systems. (3) Both the radio and the emission-line luminosity of radio AGN evolve significantly with redshift. The average [O III] rest equivalent width increases by 1 dex from z = 0.2 to z = 0.6, and emission-line ratios change from LINER-like at low redshift to Seyfert-like at high redshift. However, radio galaxies with similar stellar population parameters have similar emission-line properties both at high and at low redshift. These results suggest that massive galaxies experience cyclical episodes of gas accretion, star formation and black hole growth, followed by the production of a radio jet that shuts down further activity. The behaviour of galaxies with log M * /M > 11.4 is the same at z = 0.6 as it is at z = 0.2, except that higher redshift galaxies experience more star formation and black hole growth and produce more luminous radio jets during each accretion cycle.
MNRAS , 2019
Here we explore the infrared (IR) properties of the progenitors of high-z quasar host galaxies. Adopting the cosmological, data constrained semi-analytic model GAMETE/QSOdust, we simulate several independent merger histories of a luminous quasar at z ~ 6, following black hole growth and baryonic evolution in all its progenitor galaxies. We find that a fraction of progenitor galaxies (about 0.4 objects per single luminous quasar) at 6.5 < z < 8 has an IR luminosity of L_IR > 10^13 Lsun (hyper-luminous IR galaxies; HyLIRGs). HyLIRGs progenitors reside in the most massive halos, with dark matter (DM) masses of M_DM ~ 10^12.5 - 10^13 Msun. These systems can be easily observed in their ~ 1 mm-continuum emission in a few seconds of integration time with the Atacama Large Millimeter/submillimeter Array (ALMA), and at least 40% of them host nuclear BH activity that is potentially observable in the soft and hard X-ray band. Our findings are in line with recent observations of exceptional massive DM halos hosting HyLIRGs at z ~ 7, suggesting that z ~ 6 luminous quasars are indeed the signposts of these observed rare peaks in the high-z cosmic density field, and that massive IR-luminous galaxies at higher z are their natural ancestors.
Monthly Notices of …, 2011
Using 100 µm and 160 µm fluxes from GOODS-Herschel -the deepest survey yet undertaken by the Herschel telescope -we explore the infrared properties of X-ray selected active galactic nuclei (AGNs) up to z ≈ 3. We show that the observed 100 µm and 160 µm fluxes are dominated by emission from the host galaxy in the vast majority of cases (i.e., > 94 per cent), meaning that these far-infrared fluxes provide an uncontaminated view of the star formation in the host galaxies. There is no clear evidence of any correlation between the levels of nuclear and star formation activity at all surveyed redshifts. On the other hand, we confirm that the star formation rates of AGN hosts increase strongly with redshift; by a factor of 43 +27 −18 from z < 0.1 to z = 2 − 3 for AGNs with the same range of X-ray luminosities (L X = 10 42 -10 44 ergs s −1 ). This increase is entirely consistent with the factor of 25-50 increase in the specific star formation rates (SSFRs) of normal, star-forming (i.e., main-sequence) galaxies over the same redshift range. Indeed, the average SSFRs of AGN hosts are only marginally (i.e., ≈ 20 per cent) lower than those of main-sequence galaxies at all surveyed redshifts. We estimate that between 79 ± 10 per cent of moderate luminosity (L X = 10 42 -10 44 ergs s −1 ) AGNs are hosted in main-sequence galaxies, 15 ± 7 per cent in quiescent galaxies and < 10 per cent in strongly starbursting galaxies. We derive the fractions of all main sequence galaxies at z < 2 that are experiencing a period of moderate nuclear activity, noting that it is strongly dependent on galaxy stellar mass (M stars ); rising from just a few per cent at M stars ∼ 10 10 M ⊙ to 50 per cent at M stars 10 11 M ⊙ . We argue that our findings imply that the majority of moderate nuclear activity is fuelled by internal mechanisms rather than violent mergers, which suggests that high redshift disk instabilities could be an important AGN feeding mechanism.
Astrophysical Journal, 2007
We have discovered a strong damped Lyman alpha system essentially coincident in redshift with the faint QSO Q2343-BX415 (R = 20.2, z em = 2.57393). Such 'proximate' damped systems (PDLAs) are rare and deserving of further study as potential probes of the environments where AGN are found. Follow-up observations of the spectrum of Q2343-BX415 at intermediate spectral resolution reveal that the metal lines associated with the PDLA consist of two sets of absorption components. One set of components is apparently moving towards the quasar with velocities of ∼ 150 − 600 km s −1 ; this gas is highly ionized and does not fully cover the continuum source, suggesting that it is physically close to the active nucleus of the galaxy. Most of the neutral gas in the PDLA is blueshifted relative to the QSO by ∼ 160 km s −1 . We explore the possibility that the PDLA arises in the outflowing interstellar medium of the host galaxy of Q2343-BX415; we conclude that this interpretation is supported by the presence of strong C IV and N V absorption at nearby velocities (the latter in particular requiring a non-thermal ionizing source), and by the intense radiation field longward of the Lyman limit implied by the high C II * /H I ratio. If Q2343-BX415 is the main source of these UV photons, then the PDLA is located at either ∼ 8 or ∼ 37 kpc from the active nucleus. Alternatively, the absorber may be a foreground star-forming galaxy unrelated to the quasar and coincidentally at the same redshift, but our deep imaging and follow-up spectroscopy of the field of Q2343-BX415 has not yet produced a likely candidate. We measure the abundances of 14 elements in the PDLA, finding an overall metallicity of ∼ 1/5 solar and a normal pattern of relative element abundances for this metallicity, including moderate depletions of refractory elements and no overabundance of the α-capture elements relative to the Fe group (once depletions have been taken into account). Thus, in this PDLA there is no evidence for the super-solar metallicities that have been claimed for some proximate, high ionization, systems. In addition to the PDLA, our spectrum of Q2343-BX415 shows absorption by 11 intervening systems at z abs < z em ; we find possible galaxy identifications for four of them from an as yet incomplete spectroscopic survey of galaxies within ∼ 1 arcmin of the QSO sight-line.
New Astronomy Reviews, 2006
We present VLT/ISAAC near-infrared imaging of the host galaxies of 15 low luminosity quasars at 1 < z < 2. This work complements our studies to trace the cosmological evolution of the host galaxies of high luminosity quasars. The radioloud (RLQ) and radio-quiet (RQQ) quasars have similar distribution of redshift and luminosity, and together the high and low luminosity quasars cover a large range of the quasar luminosity function. Both RLQ and RQQ hosts resemble massive inactive ellipticals undergoing passive evolution. However, RLQ hosts are systematically more luminous than RQQ hosts, as also found for the high luminosity quasars. The difference in the host luminosity remains the same from z = 2 to z = 0. For the entire set of quasars, we find a correlation between the nuclear and the host luminosities, albeit with a large scatter. The correlation is less apparent for the RQQs than for the RLQs.
Monthly Notices of the Royal Astronomical Society, 2013
We present deep HST/WFPC2, rest-frame U images of 17 ∼ L ⋆ quasars at z ≈ 1 and z ≈ 2 (V and I bands respectively), designed to explore the host galaxies. We fit the images with simple axisymmetric galaxy models, including a point-source, in order to separate nuclear and host-galaxy emission. We successfully model all of the host galaxies, with luminosities stable to within 0.3 mag. Combining with our earlier NICMOS rest-frame optical study of the same sample, we provide the first rest-frame U − V colours for a sample of quasar host galaxies. While the optical luminosities of their host galaxies indicate that they are drawn purely from the most massive ( > ∼ L ⋆ ) early-type galaxy population, their colours are systematically bluer than those of comparably massive galaxies at the same redshift. The host galaxies of the radioloud quasars (RLQ) in our sample are more luminous than their radio-quiet quasar (RQQ) counterparts at each epoch, but have indistinguishable colours, confirming that the RLQ's are drawn from only the most massive galaxies (10 11 − 10 12 M ⊙ even at z ≈ 2), while the RQQ's are slightly less massive (∼ 10 11 M ⊙ ). This is consistent with the well-known anti-correlation between radio-loudness and accretion rate. Using simple stellar population "frosting" models we estimate mean star formation rates of ∼ 350 M ⊙ yr −1 for the RLQ's and ∼ 100 M ⊙ yr −1 for the RQQ's at z ≈ 2. By z ≈ 1, these rates have fallen to ∼ 150 M ⊙ yr −1 for the RLQ's and ∼ 50 M ⊙ yr −1 for the RQQ's. We conclude that while the host galaxies are extremely massive, they remain actively star-forming at, or close to, the epoch of the quasar.
Monthly Notices of the Royal Astronomical Society, 2013
Using the new evolutionary code PÉGASE.3, we undertook an evolutionary spectral synthesis of the optical-IR-submm spectral energy distribution of two distant (z = 3.8) radio galaxies, 4C 41.17 and TN J2007−1316. These two radio galaxies were selected from the HeRGÉ (Herschel Radio Galaxies Evolution) Project in particular for their faint active galactic nucleus contribution and because they show evidence of a large stellar contribution to their bolometric luminosity. PÉGASE.3 coherently models the reprocessing of the stellar luminosity to dust emission, allowing us to build UV to IR-submm spectral energy distribution libraries that can then be used to fit spectral energy distributions in the observer's frame. Our principal conclusion is that a single stellar population is insufficient to fit the spectral energy distribution of either radio galaxy. Our best fits are a sum of two evolving stellar populations-a recent starburst plus an old population-plus the thermal emission from an active galactic nucleus (which provides a good fit to the mid-IR emission). The two stellar components are: (i) a massive (10 11 M) starburst 30 Myr after formation,which is required simultaneously to fit the far-IR Herschel to submm data and the optical data; and (ii) an older massive (10 11-12 M) early-type galaxy population, 1.0 Gyr old, which is required principally to fit the mid-IR Spitzer/IRAC data. A young population alone is insufficient because an evolved giant star population produces a 1-µm rest-frame peak that is observed in the IRAC photometry. This discovery confirms that many of the stellar populations in high-redshift radio galaxies were formed by massive starbursts in the early Universe. Gas-rich mergers and/or jet-cloud interactions are favoured for triggering the intense star formation necessary to explain the properties of the spectral energy distributions. The discovery of similar characteristics in two distant radio galaxies suggeststhat multiple stellar populations, one old and one young, may be a generic feature of the luminous infrared radio galaxy population.
Symposium - International Astronomical Union
The V/Vmax test for quasars and the counts of radio sources show that the most powerful extragalactic radio sources exhibit strong evolutionary changes with cosmological epoch (see M. Schmidt and J.V. Wall et al., this volume). It should be emphasised that these are very large changes indeed. Schmidt, for example, has shown that for the world model with Ω = 0, evolution functions of the form F(t)∝exp(-10t/to) can account for the observations, to being the present epoch and t cosmic time. Since the quasar population from which this law is derived extends at least to Z = 2.5, corresponding to t = to/3.5 if Ω = 0, the comoving space density of quasars at Z = 2.5 must have been about 1300 times greater than it is at the present epoch. It is not known whether or not this law continues to hold at larger redshifts but even if it does, the increase in comoving space density from Z = 2.5 to infinity is only a further factor of 17. Therefore the bulk of the evolution occurs within the range o...
The Astronomical Journal, 2001
Deep optical images have been gathered for a nearly complete sample of radio galaxies from the Revised 3rd Cambridge (3CR) Catalog in the redshift range 0.15 < z < 0.65. Total and nuclear magnitudes and colors have been extracted. The richness of the galaxy clustering environment has also been quantified by calculating the amplitude of the galaxy-galaxy spatial covariance function (B gg), showing overdensities ranging up to Abell class 0-1 clusters. These optical data are compared to similar data from an existing sample of radio-loud quasars in the same redshift range for the purpose of determining the relationship between radio galaxies and quasars. In the range 0.15 < z < 0.4, we find that quasars and radio galaxies have significantly different environments in that only radio galaxies are found in rich cluster environments. This comparison appears to rule out the hypothesis that all quasars are radio galaxies viewed from a particular angle at the 97% confidence level (99.6% confidence level if N-galaxies are considered quasars). The existence of quasars in clusters at z > 0.4 supports the hypothesis that some radio-loud quasars may dim with time and evolve into radio galaxies with an efolding time of ∼ 0.9 Gyr. A compatible scenario is presented for this evolution in which the quasar dims due to the absence of low velocity interactions between the quasar host and companion galaxies which trigger quasar activity and/or a diminishing fuel supply caused by the more effective gas "sweeping" of a growing intracluster medium.
The Astrophysical Journal, 2013
We present optical spectroscopy of a sample of 38 post-starburst quasars (PSQs) at z ∼ 0.3, 29 of which have morphological classifications based on Hubble Space Telescope imaging. These broad-lined active galactic nuclei (AGNs) possess the spectral signatures of massive intermediate-aged stellar populations making them potentially useful for studying connections between nuclear activity and host galaxy evolution. We model the spectra in order to determine the ages and masses of the host stellar populations, and the black hole masses and Eddington fractions of the AGNs. Our model components include an instantaneous starburst, a power-law, and emission lines. We find the PSQs have M BH ∼ 10 8 M accreting at a few percent of Eddington luminosity and host ∼ 10 10.5 M stellar populations which are several hundred Myr to a few Gyr old. We investigate relationships among these derived properties, spectral properties, and morphologies. We find that PSQs hosted in spiral galaxies have significantly weaker AGN luminosities, older starburst ages, and narrow emission-line ratios diagnostic of ongoing star-formation when compared to their early-type counterparts. We conclude that the early-type PSQs are likely the result of major mergers and were likely luminous infrared galaxies in the past, while spiral PSQs with more complex star-formation -2histories are triggered by less dramatic events (e.g., harassment, bars). We provide diagnostics to distinguish the early-type and spiral hosts when high spatial resolution imaging is not available.
Monthly Notices of the Royal Astronomical Society, 2010
We study the dependence of the M BH-M host relation on the redshift up to z = 3 for a sample of 96 quasars, the host galaxy luminosities of which are known. Black hole masses were estimated assuming virial equilibrium in the broad-line regions, while the host galaxy masses were inferred from their luminosities. With these data, we are able to pin down the redshift dependence of the M BH-M host relation along 85 per cent of the Universe age. We show that, in the sampled redshift range, the M BH-L host relation remains nearly unchanged. Once we take into account the ageing of the stellar population, we find that the M BH /M host ratio () increases by a factor of ∼7 from z = 0 to z = 3. We show that evolves with z regardless of the radio loudness and of the quasar luminosity. We propose that the most massive black holes, living their quasar phase at high redshift, become extremely rare objects in host galaxies of similar mass in the Local Universe.
New Astronomy Reviews, 2006
We report on ESO-VLT adaptive optics imaging of one radio-loud quasar at z ∼ 3. In spite of the large distance of the object we are able to detect its surrounding extended nebulosity the properties of which are consistent with an underlying massive galaxy of M K ∼ -27 and effective radius R e = 7 kpc. As far as we know this is the clearest detection of a radio loud quasar host at high redshift. The host luminosity is indicative of the existence of massive spheroids even at this early cosmic epoch. The host luminosity is about 1 magnitude fainter than the expected value based on the average trend of the host galaxies of RLQ at lower redshift. The result, which however is based on a single object, suggests that at z ∼ 3 there is a deviation from a luminosity-redshift dependence regulated only by passive evolution.
The Astrophysical Journal, 2014
We present the results of a combined galaxy population analysis for the host galaxies of active galactic nuclei (AGN) identified at 0 < z < 1.4 within the SDSS, Boötes and DEEP2 surveys. We identified AGN in a uniform and unbiased manner at X-ray, infrared and radio wavelengths. Supermassive black holes undergoing radiatively-efficient accretion (detected as X-ray and/or infrared AGN) appear to be hosted in a separate and distinct galaxy population than AGN undergoing powerful mechanically dominated accretion (radio AGN). Consistent with some previous studies, radiatively efficient AGN appear to be preferentially hosted in modest star-forming galaxies, with little dependence on AGN or galaxy luminosity. AGN exhibiting radio-emitting jets due to mechanically-dominated accretion are almost exclusively observed in massive, passive galaxies. Crucially, we now provide strong evidence that the observed host-galaxy trends are independent of redshift. In particular, these different accretion-mode AGN have remained as separate galaxy populations throughout the last 9 Gyr. Furthermore, it appears that galaxies hosting AGN have evolved along the same path as galaxies that are not hosting AGN with little evidence for distinctly separate evolution.
ESO Astrophysics Symposia, 2005
We present a study of the M BH-M host relation as a function of Cosmic Time in a sample of ∼ one hundred quasars from z = 0 to 3. In this paper we describe the sample, the data sources and the new spectroscopic observations. We then illustrate how we derive M BH from single-epoch spectra, pointing out the uncertainties in the procedure and addressing the role of possible selection biases. In a companion paper, we address the dependence of the ratio between the black hole mass and the host galaxy luminosity and mass on Cosmic Time.
Monthly Notices of the Royal Astronomical Society, 2000
We present optical (∼ 3200Å to ∼ 9000Å ) off-nuclear spectra of 26 powerful active galaxies in the redshift range 0.1 ≤ z ≤ 0.3, obtained with the Mayall and William Herschel 4-meter class telescopes. The sample consists of radio-quiet quasars, radio-loud quasars (all with −23 ≥ M V ≥ −26) and radio galaxies of Fanaroff & Riley Type II (with extended radio luminosities and spectral indices comparable to those of the radio-loud quasars). The spectra were all taken approximately 5 arcseconds offnucleus, with offsets carefully selected so as to maximise the amount of galaxy light falling into the slit, whilst simultaneously minimising the amount of scattered nuclear light. The majority of the resulting spectra appear to be dominated by the integrated stellar continuum of the underlying galaxies rather than by light from the non-stellar processes occurring in the active nuclei, and in many cases a 4000Å break feature can be identified. The individual spectra are described in detail, and the importance of the various spectral components is discussed. Stellar population synthesis modelling of the spectra will follow in a subsequent paper .
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