Annu. Rev. Astron. Astrophys. 1999. 37:
127-189 Copyright © 1999 by . All rights reserved |
In this preliminary section, I do not discuss at length the theoretical basis of the gravitational lens effect because all the details can be found in the comprehensive textbook written by Schneider et al (1992). I focus on concepts and basic equations of the gravitational lensing theory, in the thin lens approximation and for small deviation angles, which are necessary for this review.
The apparent angular position of a lensed image, ^{I} (in this review, bold symbols denote vectors), can be expressed as a function of the (unlensed) angular position of the source, ^{S}, and the deflection angle, (^{I}) as follows (see Figure 1):
(1) |
(^{I}). depends on the projected mass density of the lens, (^{I}), and the cosmological parameters through the angular-diameter distances from the lens L to the source S, D_{LS}, from the observer o to the source, D_{OS}, and from the observer to the lens, D_{OL}:
(2) |
where G is the gravitational constant and c is the speed of light. (^{I}) can be expressed as a function of the Poisson equation, and the strength of the lens is characterized by the ratio of the projected mass density of the lens to its critical projected mass density _{crit} (see Fort & Mellier 1994):
(3) |
where is the 2-dimension Laplacian and is the dimensionless gravitational potential projected along the line of sight which is related to the projected gravitational potential as follows:
(4) |
From the differentiation of Equation (1), we can express the deformation of an infinitesimal ray bundle as a function of the Jacobian
(5) |
where A(^{I}) is the magnification matrix:
(6) |
It can be written as a function of two parameters (similar to the magnification and the astigmatism terms in classical optics), the convergence, , and the shear components _{1} and _{2} of the complex shear = _{1} + i _{2}:
(7) |
The isotropic component of the magnification, = 1/2 (^{I}), is directly related to the projected mass density, and the two components _{1} and _{2} describe an anisotropic deformation produced by the tidal gravitational field. The eigenvalues of the magnification matrix are 1 - ± ||, where || = (_{1}^{2} + _{2}^{2})^{1/2}. They provide the elongation and the orientation produced on the images of lensed sources. The magnification of an image is:
(8) |
The points of the image plane where det (A) = 0 are called the critical lines. The corresponding points of the source plane are called the caustic lines and produce infinite magnification (see Schneider et al 1992;, Blandford & Narayan 1992;, Fort & Mellier 1994 for more detailed descriptions of caustic and critical lines). The strong lensing cases correspond to configurations where sources are close to the caustic lines. These lenses have (^{I}) / _{crit} 1 and the convergence and shear are strong enough to produce giant arcs and multiple images for suitably positioned sources (Figures 2 and 3). The weak lensing regime, which is the main topic of this review, corresponds to lensing configurations where << 1 and << 1. In this regime, the magnification and the distortion of background galaxies are so small that they cannot be detected on individual objects. In that case, it is necessary to analyze statistically the distortion of the lensed population.
Figure 1. Description of a lensing configuration. |
Figure 3. A panel of lensing clusters observed with HST. The arc(let)s and multiple lensed images are indicated by a letter. In A2390 (top left), the straight arc is made of two different galaxies corresponding to images A and C. The pairing of some images is obvious, like B in A2390 (top-left), A in AC114, or A in A370. Image B in MS2137 and B in A370 are radial arcs. A in MS2137 is a triple image from an almost ideal configuration of a fold caustic. |