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and Cosmology

Extragalactic Astronomy and Cosmology: An Introduction

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3. The World of Galaxies<br />

128<br />

Fig. 3.38. Left: milliarcsecond structure of the two images<br />

of the quasar QSO 0957+561, a VLBI map at 13 cm<br />

wavelength by Gorenstein et al. Both quasar images show<br />

a core-jet structure, <strong>and</strong> it is clearly seen that they are mirrorsymmetric,<br />

as predicted by lens models. right: spectra of<br />

the two quasar images QSO 0957+561A,B, observed by the<br />

Faint Object Camera (FOC) on-board HST. The similarity<br />

of the spectra, in particular the identical redshift, is a clear<br />

indicator of a common source of the two quasar images.<br />

The broad Lyα line, in the wings of which an NV line is<br />

visible, is virtually always the strongest emission line in<br />

quasars<br />

The mass within θ E of a lens follows from the fact<br />

that the mean surface mass density within θ E equals<br />

the critical surface mass density Σ cr . A more accurate<br />

determination of lens masses is possible by<br />

means of detailed lens models. For quadruple image<br />

systems, the masses can be derived with a precision<br />

of a few percent – these are the most precise mass<br />

determinations in (extragalactic) astronomy.<br />

QSO 2237+0305: The Einstein Cross. A spectroscopic<br />

survey of galaxies found several unusual emission lines<br />

in the nucleus of a nearby spiral galaxy which cannot<br />

originate from this galaxy itself. Instead, they are<br />

emitted by a background quasar at redshift z s = 1.7 situated<br />

exactly behind this spiral. High-resolution images<br />

show four point sources situated around the nucleus<br />

of this galaxy, with an image separation of Δθ ≈ 1 . ′′ 8<br />

(Fig. 3.40). The spectroscopic analysis of these point<br />

sources revealed that all four are images of the same<br />

quasar (Fig. 3.41).<br />

The images in this system are positioned nearly symmetrically<br />

around the lens center; this is also a typical<br />

lens configuration which may be caused by an elliptical<br />

lens (see Fig. 3.36). The Einstein radius of this lens<br />

is θ E ≈ 0 . ′′ 9, <strong>and</strong> we can determine the mass within this<br />

radius with a precision of ∼ 3%.<br />

Einstein Rings. More examples of Einstein rings are<br />

displayed in Figs. 3.42 <strong>and</strong> 3.43. The first of these<br />

is a radio galaxy, with its two radio components be-

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