Type 1 AGN at low z. II. The relative strength of narrow lines and the nature of intermediate type AGN

TL;DR

This study investigates how the strength of narrow emission lines in low-redshift Type 1 AGN varies with luminosity, revealing a decrease in narrow line contribution at higher luminosities and implications for AGN classification and structure.

Contribution

It provides a detailed analysis of the luminosity dependence of narrow line emission in Type 1 AGN, highlighting the decreasing narrow line region covering factor with increasing bolometric luminosity.

Findings

Narrow to broad H-alpha luminosity ratio decreases with increasing luminosity.

Bolometric correction factor for [OIII] emission decreases at higher luminosities.

Most low-luminosity AGN appear as intermediate type due to dominant narrow lines.

Abstract

We explore the relative strength of the narrow emission lines in an SDSS based sample of broad H-alpha selected AGN, defined in paper I. We find a decrease in the narrow to broad H-alpha luminosity (L_bHa) ratio with increasing L_bHa, such that both L([OIII] lambda5007) and L(narrow H-alpha) scale as L_bHa^0.7 for 10^40 < L_bHa < 10^45 ergs s^-1. Following our earlier result that L_bHa \propto L_bol, this trend indicates that the relative narrow line luminosity decreases with increasing L_bol. We derive L_bol / 10^43 ergs s^-1 = 4000 (L([OIII]) / 10^43 ergs s^-1)^1.39. This implies that the bolometric correction factor, L_bol / L([OIII]), decreases from 3,000 at L_bol = 10^46.1 ergs s^-1 to 300 at L_bol = 10^42.5 ergs s^-1. At low luminosity, the narrow component dominates the observed H-alpha profile, and most type 1 AGN appear as intermediate type AGN. Partial obscuration or extinction cannot explain the dominance of intermediate type AGN at low luminosity, and the most likely mechanism is a decrease in the narrow line region covering factor with increasing L_bol. Deviations from the above trend occur in objects with L / L_Edd <~ 10^-2.6, probably due to the transition to LINERs with suppressed [OIII] emission, and in objects with M_BH > 10^8.5 M_Sun, probably due to the dominance of radio loud AGN, and associated enhanced [OIII] emission.