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and Cosmology

Extragalactic Astronomy and Cosmology: An Introduction

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5.4 Components of an AGN<br />

by magnetic fields, or even gravitationally. One possibility<br />

is that the clouds are the extended atmospheres<br />

of stars; this would, however, imply a very high (too<br />

high?) total mass of the BLR.<br />

5.4.3 Narrow Emission Lines<br />

Besides the broad emission lines that occur in QSOs,<br />

Seyfert 1 galaxies, <strong>and</strong> broad-line radio galaxies, most<br />

AGNs (with exception of the BL Lacs) show narrow<br />

emission lines. Their typical width is ∼ 400 km/s. This<br />

is considerably narrower than lines of the BLR, but<br />

still significantly broader than characteristic velocities<br />

in normal galaxies. In analogy to the BLR, the region in<br />

which these lines are produced is known as the narrow<br />

line region (NLR). The strongest line from the NLR<br />

is, besides Lyα <strong>and</strong> CIV, the forbidden [OIII] line at<br />

λ = 5007 Å. The existence of forbidden lines implies<br />

that the gas density in the NLR is significantly lower<br />

than in the BLR. From estimates analogous to those<br />

for the BLR, the characteristic properties of the NLR<br />

are determined. It should be noted that no reverberation<br />

mapping can be applied, since the extent of the NLR<br />

is ∼ 100 pc. Because of this large extent, no variability<br />

of the narrow line intensities is expected on time-scales<br />

accessible to observation, <strong>and</strong> none has been found.<br />

The line ratios of allowed <strong>and</strong> forbidden lines yield<br />

n e ∼ 10 3 cm −3 for the typical density of the gas in which<br />

the lines originate. The characteristic temperature of the<br />

gas is likewise obtained from line ratios, T ∼ 16 000 K,<br />

which is slightly lower than in the BLR. The filling<br />

factor here is also significantly smaller than one, about<br />

10 −2 . Hence, the geometrical picture of clouds in the<br />

NLR also emerges. Like in the BLR, the properties of<br />

the NLR are not homogeneous but vary with r.<br />

Since the extent of the NLR in Seyfert galaxies is of<br />

the order of r ∼ 100 pc, it can be spatially resolved for<br />

nearby Seyfert galaxies. The morphology of the NLR is<br />

very interesting: it is not spherical, but appears as two<br />

cone-shaped regions (Fig. 5.24). It seems as if the ionization<br />

of the NLR by the continuum radiation of the<br />

AGN is not isotropic, but instead depends strongly on<br />

the direction.<br />

5.4.4 X-Ray Emission<br />

The most energetic radiation of an AGN is expected to<br />

be produced in the immediate vicinity of the SMBH.<br />

201<br />

Fig. 5.24. Image of the Seyfert galaxy NGC 5728. Left:<br />

a large-scale image showing the disk galaxy; right: an HST<br />

image of its central region taken through a filter with a small<br />

b<strong>and</strong>width (narrow-b<strong>and</strong> filter) centered on a narrow emission<br />

line. This image shows the spatially resolved NLR. We can<br />

see that it is not spherical but consists of two cones. From this,<br />

it is concluded that the ionizing radiation of the AGN is not<br />

isotropic, but is emitted in two preferred directions perpendicular<br />

to the disk of the Galaxy (<strong>and</strong> thus probably perpendicular<br />

to the central accretion disk)

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