73 research outputs found

    The sizes of BLRs and BH masses of double-peaked broad low-ionization emission line objects

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    In this paper, the sizes of the BLRs and BH masses of DouBle-Peaked broad low-ionization emission line emitters (dbp emitters) are compared using different methods: virial BH masses vs BH masses from stellar velocity dispersions, the size of BLRs from the continuum luminosity vs the size of BLRs from the accretion disk model. First, the virial BH masses of dbp emitters estimated by the continumm luminosity and line width of broad Hβ\beta are about six times (a much larger value, if including another dbp emitters, of which the stellar velocity dispersions are traced by the line widths of narrow emission lines) larger than the BH masses estimated from the relation MBH−σM_{BH} - \sigma which is a more accurate relation to estimate BH masses. Second, the sizes of the BLRs of dbp emitters estimated by the empirical relation of RBLR−L5100A˚R_{BLR} - L_{5100\AA} are about three times (a much larger value, if including another dbp emitters, of which the stellar velocity dispersions are traced by the line widths of narrow emission lines) larger than the mean flux-weighted sizes of BLRs of dbp emitters estimated by the accretion disk model. The higher electron density of BLRs of dbp emitters would be the main reason which leads to smaller size of BLRs than the predicted value from the continuum luminosity.Comment: 7 pages, two figures and one table. Accepted by MNRA

    The Correlation Between Spectral Index And Accretion Rate For AGN

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    In this paper, we present a correlation between the spectral index distribution (SED) and the dimensionless accretion rate defined as m˙=Lbol/LEdd\dot{m}={L_{bol}/L_{Edd}} for AGN. This quantity is used as a substitute of the physical accretion rate. We select 193 AGN with both broad Hα\alpha and broad Hβ\beta, and with absorption lines near MgIλ5175A˚\lambda5175\AA from SDSS DR4. We determine the spectral index and dimensionless accretion rate after correcting for both host galaxy contribution and internal reddening effects. A correlation is found between the optical spectral index and the dimensionless accretion rate for AGN, including low luminosity AGN (LHα<1041erg⋅s−1L_{H\alpha}<10^{41}{\rm erg\cdot s^{-1}} sometimes called "dwarf AGN" (Ho et al. 1997)). The existence of this correlation provides an independent method to estimate the central BH masses for all types of AGN. We also find that there is a different correlation between the spectral index and the BH masses for normal AGN and low luminosity AGN, which is perhaps due to the different accretion modes in these two types of nuclei. This in turn may lead to the different correlations between BH masses and optical continuum luminosity reported previously (Zhang et al. 2007a), which invalidates the application of the empirical relationship found by Kaspi et al. (2000, 2005) to low luminosity AGN in order to determine their BLR sizes.Comment: 10 pages, 7 figures, accepted for publication in MNRA

    GTC Spectra of z ~ 2.3 Quasars: Comparison with Local Luminosity Analogues

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    [Abridged] Context: The advent of 8-10m class telescopes makes possible for the first time detailed comparison of quasars with similar luminosity and very different redshifts. Aims: A search for z-dependent gradients in line emission diagnostics and derived physical properties by comparing, in a narrow bolometric luminosity range (log L ~ 46.1 +/- 0.4 [\ergss]), some of the most luminous local (z < 0.6) quasars with some of the lowest luminosity sources yet found at redshift z = 2.1 ~ 2.5. Method: Spectra for 22 high z sources were obtained with the 10.4m Gran Telescopio Canarias (GTC) while the HST (largely FOS) archive provides a low redshift control sample. Comparison is made in the context of the 4D Eigenvector 1 formalism meaning that we divide both source samples into high accreting Population A and low accreting Population B sources. Results: CIV 1549 shows very similar properties at both redshifts confirming at high redshift the CIV profile differences between Pop. A and B that are well established in local quasars. The CIV blueshift that appears quasi- ubiquitous in higher L sources is found in only half (Pop. A) of quasars observed in both of our samples. A CIV evolutionary Baldwin effect is certainly disfavored. We find evidence for lower metallicity in the GTC sample that may point toward a gradient with z. No evidence for a gradient in black hole mass or Eddington ratio is found. Conclusions: Spectroscopic differences established at low redshift are also present in much higher redshift quasars. Given that our samples involve sources with very similar luminosity the evidence for a systematic metallicity decrease, if real, points toward an evolutionary effect. Our samples appear representative of a slow evolving quasar population likely present at all redshifts.Comment: To appear in Astronomy & Astrophysic

    The size of BLRs of low luminous Active Galactic Nuclei

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    We study the size of BLRs of low luminosity Active Galactic Nuclei, also called 'dwarf AGN', defined as having (LHα≤1041erg⋅s−1L_{H\alpha}\le10^{41}{\rm erg\cdot s^{-1}})). We more than double the sample size analyzed previously (Wang & Zhang 2003, hereafter Paper I). In this study we first confirm our previous result that the sizes of BLRs of low luminosity AGN are larger than the ones expected from the empirical relation RBLRs−LHαR_{BLRs} - L_{H\alpha} valid for 'normal' AGN: Seyfert 1s and quasars, except for the objects with accretion rate mHα˙>10−5.5\dot{m_{H\alpha}}>10^{-5.5}. Second, we find a positive correlation between the line width of the narrow emission line (as tracer of velocity dipersion and thus bulge and black hole mass) and the size of BLRs for both normal and low luminosity AGN. In this paper we find a non-linear dependence of the BLRs sizes of low luminosity AGN on BH masses. We also show that their sizes of BLRs are more strongly dominated by the 'specific accretion rate' mHα˙\dot{m_{H\alpha}} defined as mHα˙=LHα/LEdd\dot{m_{H\alpha}} = L_{H\alpha}/L_{Edd}, than by the masses of their cetral black holes. As an expected result, the distance of emission regions of low-ionization broad Hα\alpha of NGC 4395 should be consistent with the value from the empirical relation of RBLRs−LHαR_{BLRs} - L_{H\alpha}, according to the high accretion rate.Comment: Accepted by MNRA
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