The physical driver of the optical Eigenvector 1 in Quasar Main Sequence
arXiv:1710.10180 · doi:10.3389/fspas.2017.00033
Abstract
Quasars are complex sources, characterized by broad band spectra from radio through optical to X-ray band, with numerous emission and absorption features. However, Boroson & Green (1992) used Principal Component Analysis (PCA), and with this analysis they were able to show significant correlations between the measured parameters. The leading component, related to Eigenvector 1 (EV1) was dominated by the anticorrelation between the Fe optical emission and [OIII] line and EV1 alone contained 30% of the total variance. It opened a way in defining a quasar main sequence, in close analogy to the stellar main sequence on the Hertzsprung-Russel (HR) diagram (Sulentic et al. 2001). The question still remains which of the basic theoretically motivated parameters of an active nucleus (Eddington ratio, black hole mass, accretion rate, spin, and viewing angle) is the main driver behind the EV1. Here we limit ourselves to the optical waveband, and concentrate on theoretical modelling the Fe to H ratio, and we test the hypothesis that the physical driver of EV1 is the maximum of the accretion disk temperature, reflected in the shape of the spectral energy distribution (SED). We performed computations of the H and optical Fe for a broad range of SED peak position using CLOUDY photoionisation code. We assumed that both H and Fe emission come from the Broad Line Region represented as a constant density cloud in a plane-parallel geometry. We expected that a hotter disk continuum will lead to more efficient production of Fe but our computations show that the Fe to H ratio actually drops with the rise of the disk temperature. Thus either hypothesis is incorrect, or approximations used in our paper for the description of the line emissivity is inadequate.
arXiv comment12 pages, 4 figures, Accepted for publication in the Journal Frontiers in Astronomy and Space Sciences
References in corpus (24)
- Spectral Energy Distributions and Multiwavelength Selection of Type 1 Quasars
- The Low-Luminosity End of the Radius-Luminosity Relationship for Active Galactic Nuclei
- Systematic Effects in Measurement of Black Hole Masses by Emission-Line Reverberation of Active Galactic Nuclei: Eddington Ratio and Inclination
- The diversity of quasars unified by accretion and orientation
- Eigenvector 1: An Optimal Correlation Space for Active Galactic Nuclei
- The origin of the Broad Line Region in Active Galactic Nuclei
- Spectral Classification of Quasars in the Sloan Digital Sky Survey: Eigenspectra; Redshift and Luminosity Effects
- CIV 1549 as an Eigenvector 1 Parameter for Active Galactic Nuclei
- Average Quasar Spectra in the Context of Eigenvector 1
- An X-shooter composite of bright 1 < z < 2 quasars from UV to infrared
- Active galactic nuclei at z ~ 1.5: I. Spectral energy distribution and accretion discs
- Self-shadowing Effects of Slim Accretion Disks in Active Galactic Nuclei: Diverse Appearance of the Broad-line Region
- Accretion Disk Temperatures and Continuum Colors in QSOs
- Dissecting the quasar main sequence: insight from host galaxy properties
- Constraints on the black hole spin in the quasar SDSS J094533.99+100950.1
- Active galactic nuclei at z ~ 1.5: III. Accretion discs and black hole spin
- The dust origin of the Broad Line Region and the model consequences for AGN unification scheme
- PCA of the spectral energy distribution and emission line properties of red 2MASS AGN
- The mass of the black hole in RE J1034+396
- Fe II Emission in AGN: The Role of Total and Gas-Phase Iron Abundance
- The properties of active galaxies at the extreme of eigenvector 1
- Absorption features in the quasar HS 1603+3820 II. Distance to the absorber from photoionisation modelling
- UV spectral diagnostics for low redshift quasars: estimating physical conditions and radius of the Broad Line Region
- Extending the Eigenvector 1 Space to the Optical Variability of Quasars
Cited by in corpus (7)
- The Quasar Main Sequence explained by the combination of Eddington ratio, metallicity and orientation
- Modelling of the quasar main sequence in the optical plane
- The CaFe Project: Optical Fe II and Near-Infrared Ca II triplet emission in active galaxies: (I) Photoionization modelling
- Exploring the Diversity of Type 1 Active Galactic Nuclei Identified in SDSS-IV/SPIDERS
- Evolution of quasar stochastic variability along its main sequence
- High Eddington quasars as discovery tools: current state and challenges
- Quasar main sequence in the UV plane