Active galactic nuclei (AGN) display an extreme range in the narrow emission line equivalent widths. Specifically, in the PG quasar sample the equivalent width of the narrow [Oiii] λ5007 line has a range of> 300 (< 0.5˚A to 157˚A), while the broad Hβ line, for example, has a range of ten only (23˚A to 230˚A). The strength of [Oiii] λ5007 is modulated by the covering factor (CF) of the narrow line region (NLR) gas, its density (ne), and ionization parameter (U). To explore which of these factors produces the observed large range in [Oiii] λ5007 strength, we measure the strength of the matching narrow Hβ and [Oiii] λ4363 lines, detected in 40 out of the 87 z < 0.5 PG quasars in the Boroson & Green sample. The photoionization code CLOUDY is then used to infer CF, ne, and U in each object, assuming a single uniform emitting zone. We find that the range of CF ( ∼ 0.02 − 0.2) contributes about twice as much as the range in both ne and U towards modulating the strength of the [Oiii] λ5007 line. The CF is inversely correlated with luminosity, but it is not correlated with L/LEdd as previously speculated. The single zone [Oiii] λ5007 emitting region is rather compact, having RNLR = 40L0.45 pc. These emission lines can also be fit with an extreme two zone 44 model, where [Oiii] λ4363 is mostly emitted by a dense (ne = 107 cm−3) inner zone at Rin NLR = L0.5 44 pc, and [Oiii] λ5007 by a low density (ne = 103 cm−3) extended outer zone at Rout NLR = 750L0.34 44 pc. Such an extended [Oiii] λ5007 emission should be well resolved by Hubble Space Telescope imaging of luminous AGN. Further constraints on the radial gas distribution in the NLR can be obtained from the spectral shape of the IR continuum emitted by the associated dust.
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Baskin et al. (2005) studied this question.
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