Gravitational Lensing III: 

     The Weak Lensing Effect


 

Principle of the Weak Lens Effect

Multiple images, Einstein rings, and arcs are spectacular gravitational lens events. In addition to these phenomena of the so-called strong lens effect, there is also the weak gravitational lens effect, which has been known for around 10 years. This is because light bundles from very distant galaxies are not only deflected as a whole, but will also be distorted due to the tidal part of the gravitational field caused by mass inhomogeneities. This distortion is in general rather weak, and thus it cannot be found in individual objects since the intrinsic form of the sources is unknown. However, a large number density of galaxies can be found in deep optical images of the sky: up to a magnitude of R<25, there are about 35 galaxies per square arcminute, whose characteristic redshift is around z=1. Images of neighboring galaxies will be distorted by a similar tidal field. Thus if the fact that the instrinsic orientation of galaxies is random is used, then this tidal field can be determined from the average alignment of the observable images of galaxies. Conclusions about the distribution of mass can be drawn from the tidal field. Indeed, by measuring this field of distortion, the distribution of mass in a cluster of galaxies can be reconstructed, and one thus obtains a picture of (primarily dark) matter -- it really can be seen! Fig.2 shows an example of such a reconstruction of mass.
 
 

Fig.1: An image of galaxy cluster A1689 taken by the Hubble Space Telescope. A very large number of arcs can be seen around the center of this cluster, tangentially-aligned, distorted images of background galaxies. While the arcs show an increasingly smaller axis ratio away from the center, there are more of them. Further outside, the individual arclets can no longer be identified as such. However, by observing groups of images of galaxies far from the centre of the cluster, their average distortion can still be determined. The strength of the distortion is a measure of the strength of the tidal field, and the tidal field is a measure of the mass of the galaxy cluster.


Fig.2: A deep image of galaxy cluster Cl0939+4713 at z=0.41 (upper panel, taken with HST) was analysed with regard to the distortion of the weak, faint images of the background galaxies. In this manner, the tidal field of this cluster could be determined, and from it the distribution of mass could be reconstructed (lower panel). One can clearly see the center of the cluster as the maximum of the mass density, an additional (secondary) maximum, as well as a decrease in density away from the center, and a pronounced minimum. A comparison of the map of the mass with the distribution of the brighter (cluster) galaxies shows that they are very similarly distributed: the maximum in the center, the secondary maximum, as well as the minimum of the mass distribution can again be found in the distribution of the galaxies.


Fig.3: Even a cluster with a large redshift can be examined using this weak lens-effect technique. Here an image of cluster MS1054-03 with redshift z=0.83 is shown (upper panel), as well as the mass distribution determined via the weak lens effect (lower panel). Both the distribution of galaxies in the cluster (visible here as reddish galaxies) and the distribution of mass show a pronounced substructure; the cluster seems to be composed of three components. Since we see the cluster when the universe is only half as old as it is today, the cluster is very young and possibly just being formed. It may amalgamate out of three smaller clusters, which can still be seen here individually. In this way, the lens effect makes it possible to directly study the formation of structures in the universe.
 

 
 
 
 
 
 

Do Dark Clusters Exist?

With the weak lensing effect it is possible not only to analyse known galaxy clusters, but also to deliberately attempt to find them. A statistically significant alignment of the images of very distant galaxies around a point indicates the presence of a concentration of mass. In this manner, it is possible to find concentrations of mass without resorting to their properties of luminosity. This is of general cosmological interest. While the theory of structure formation makes very detailed predictions about the distribution of matter (e.g. with numerical simulations), predictions about characteristics of luminosity (galaxy development, hot gas in clusters) can be made only by using simplified assumptions and thus have a much greater degree of uncertainty. The possibility of discovering galaxy clusters or their dark matter without resorting to an excess of galaxies on optical images, or through their x-ray luminosity, would permit a direct comparison of the number density of clusters and their masses with cosmological models. Since the number density of galaxy clusters as a function of mass and redshift is a sensitive measure of the cosmological model, this comparison is of exceptional interest. Indeed, a galaxy cluster has already been discovered using this method (Fig. 4).

Fig.4: An examination of galaxy cluster A1942 using the weak lensing effect found not only the cluster itself, but also a concentration of matter whose tidal field can be proven unequivocally. The density contours of the reconstructed surface mass density placed over a deep image in the V band (left panel, field dimension is 14'x14') and in the I band (right panel, 7.5'x15') respectively are shown here. Galaxy cluster A1942 with redshift z = 0.22 can be found near the center of the V-band image and close to the upper edge in the I-band image. About 7' south of the center of the cluster, a second concentration of mass can be seen which through several statistical tests proves to be just as significant as cluster A1942 itself. No over-density of galaxies associated with this concentration of --> --mass can be seen whatsoever. It is probably a high redshift galaxy cluster which does not contain very luminous galaxies.
 

 
 
 
 
 
 

Cosmic Shear

When atoms were first being formed out of electrons and nuclei, dark matter was scattered almost homogeneously throughout the universe - almost, but not completely, as can be clearly seen from fluctuations of the cosmic microwave background radiation. From these small fluctuations in density, the large-scale distribution of material in the universe developed in the course of cosmic evolution. This can now be simulated very precisely by using super-computers - but can the large-scale structure of dark matter be observed directly? The weak lensing effect can be used here as a unique tool: bundles of light from distant sources will be become weak because of the large-scale distribution of matter, but in principle measurably distorted (cosmic shear). Using the statistical characteristics of the ellipticity distribution of galaxy images in a wide-angle image, the statistical characteristics of the distribution of dark matter can be deduced. For many years, several research groups in different countries have been looking for this effect. The difficulty lies in the minuteness of the effect: practically each inaccuracy in an image taken with a telescope yields a larger signal than from the cosmic shear itself. Only after learning how to avoid making such imaging mistakes or after learning how to correct them, four groups published their discovery almost simultaneously in March 2000. Thus for the first time, dark matter was directly observed outside bound structures such as galaxy clusters. This breakthrough will lead to cosmic shear becoming a main area of study in cosmology within the next few years. With its help, one will be able to study in detail the development of the distribution of matter and use models to compare results.
 
 

Fig.5: Here the principle of cosmic shear is shown via the propagation of light bundles (yellow) through a model of the large-scale distribution of matter in the universe, generated through simulations. Due to the distortion by the tidal fields caused by the distribution of matter, the shape of the observed image of a source (blue, to the right of the ``cube") deviates from the unlensed source (blue, to the left of the ``cube"). The statistical characteristics of the shapes of the images allows us to make direct conclusions about the statistical characteristics of the large-scale distribution of matter.
Fig.6: In this image, a measurement for cosmic shear as a function of the angular scale is displayed. The four different symbols in the diagram show the results of four different groups which independently, but almost simultaneously, achieved the breakthrough in measuring cosmic shear. It can be seen that the results of the groups agree to a large degree, which strengthens our faith in the accuracy of the measurements. The signal expected from theory is shown as dotted curves for two cosmological models. These measurements exclude with a high probability the model that is indicated by the upper curve.



Gravitational Lenses I   : Galaxies as Lenses

Gravitational Lenses II : Galaxy Clusters as Lenses