Abstract

We use high spectral resolution (R > 8000) data covering 3800-13000\r{A} to study the physical conditions of the broad line region (BLR) of nine nearby Seyfert 1 galaxies. Up to six broad HI lines are present in each spectrum. A comparison - for the first time using simultaneous optical to near-infrared observations - to photoionisation calculations with our devised simple scheme yields the extinction to the BLR at the same time as determining the density and photon flux, and hence distance from the nucleus, of the emitting gas. This points to a typical density for the HI emitting gas of 10$^{11}$cm$^{-3}$ and shows that a significant amount of this gas lies at regions near the dust sublimation radius, consistent with theoretical predictions. We also confirm that in many objects the line ratios are far from case B, the best-fit intrinsic broad-line H$\alpha$/H$\beta$ ratios being in the range 2.5-6.6 as derived with our photoionization modeling scheme. The extinction to the BLR, based on independent estimates from HI and HeII lines, is A$_V$ $\le$ 3 for Seyfert 1-1.5s, while Seyfert 1.8-1.9s have A$_V$ in the range 4-8. A comparison of the extinction towards the BLR and narrow line region (NLR) indicates that the structure obscuring the BLR exists on scales smaller than the NLR. This could be the dusty torus, but dusty nuclear spirals or filaments could also be responsible. The ratios between the X-ray absorbing column N$_H$ and the extinction to the BLR are consistent with the Galactic gas-to-dust ratio if N$_H$ variations are considered.

Highlights

  • The broad emission lines observed in the spectra of type 1 active galactic nuclei (AGNs), including the partially obscuredC 2016 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Societybroad-line region (BLR) comprises gas clouds covering a wide range of physical conditions; and line emission may arise from different regions of the ensemble according to where it is most optimally generated

  • With the exception of MCG–05-23-16, for which the photon flux is poorly constrained as it was estimated based on only three line ratios, and NGC 4235, which have the lowest photon flux in the sample, the distances are consistent with a significant amount of the H I emitting gas being located at regions near the dust sublimation radius

  • We find that in six of the nine objects in our sample, the extinction to BLR and narrow-line region (NLR) are the same within errors. We attribute this difference to Heard & Gaskell (2016) adopting a single intrinsic broad Hα/H β line ratio of 2.78 for all AGN in their analysis, which will result in overestimating the extinction to the BLR in many sources, as our analysis indicates that the intrinsic broad Hα/H β ratio has a broad distribution and is usually larger than this value

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Summary

INTRODUCTION

The broad emission lines observed in the spectra of type 1 active galactic nuclei (AGNs), including the partially obscured. On the other hand, Baron et al (2016) analysed 5000 SDSS type 1 AGNs at z ≈ 0.4 and while they found that the majority of the objects in their sample are reddened, in unreddened objects the mean Hα/H β ratio is ≈3 with a broad distribution in the range 1.5–4, which suggests that simple Case B recombination cannot explain the ratio in all sources Ruff et al (2012) took a step in this direction, using observations of optical and near-infrared (NIR) broad lines in four optically selected quasars – these were not obtained simultaneously These authors compared the observed ratios to a grid of photoionization models, in order to derive the best-fitting density and photon flux.

Sample selection
Observations
Data reduction
DATA ANALYSIS
Emission line fitting
Fe II subtraction
Subtraction of broad He I λ4922 Å
Narrow component subtraction
Fitting the broad hydrogen lines
Photoionization models
Extinction measurements
Seyfert sub-types
DISCUSSION
Predicted line ratios
Comparison of extinction to previous studies
X-ray absorption and optical extinction
Findings
Seyfert sub-type and extinction to the BLR
SUMMARY AND CONCLUSIONS
Full Text
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