Deriving Amplification of Images in Schwartzschild Metric

In summary, the paper "Strong field limit of black hole gravitational lensing" discusses the amplification of images in the Schwartzschild metric. The authors provide an equation (30) for the amplification factor, but do not explain its origin. The equation is related to equation (2) and references from the paper provide more information on these quantities.
  • #1
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In the paper Strong field limit of black hole gravitational lensing, the amplification of images in the Schwartzschild metric was given by

$$
\frac{1}{\beta}\sqrt{\frac{2\,D_{LS}}{D_{OL}D_{OS}}}
$$However the authors did not derive this expression or explain its origin. Does anyone know how to derive this expression or knows where the author got it from?

Any help is appreciated.

Thanks in advance.
 
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  • #2
I'm not well versed in gravitational lensing... I'm just looking at the form of the equations and googling some of the paper's references.

Using the paper, it seems that this equation (30) looks like it is related to equation (2) since 4GM/c^2=2(2GM/c^2).
But I have no intuition with these quantities ##\beta##, ##\theta##, ##\mu##, etc...

Possibly useful:
http://astro.psu.edu/users/rbc/a504/gravitational_lens.pdf
...apparently extracted from the paper's first reference [Schneider, Ehlers, Falco].
 

1. What is the Schwartzschild metric?

The Schwartzschild metric is a mathematical formula used in general relativity to describe the curvature of spacetime in the presence of a non-rotating, spherically symmetric mass. It is named after the German physicist Karl Schwartzschild, who first derived the metric in 1915.

2. How does the Schwartzschild metric affect the amplification of images?

The Schwartzschild metric predicts that light rays will bend as they pass through regions of strong gravitational fields, such as those near massive objects like stars or black holes. This bending of light can result in the amplification or distortion of images from distant objects, a phenomenon known as gravitational lensing.

3. What factors influence the level of amplification in the Schwartzschild metric?

The level of amplification in the Schwartzschild metric is influenced by several factors, including the mass and distance of the object causing the gravitational field, the distance between the object and the observer, and the angle at which the light rays pass through the gravitational field. The closer the object and the larger its mass, the stronger the gravitational lensing effect will be.

4. How is the amplification of images calculated in the Schwartzschild metric?

The amplification of images in the Schwartzschild metric can be calculated using the lens equation, which takes into account the distance between the object and the observer, the distance between the object and the lensing mass, and the mass of the lensing object. This equation is based on the principles of gravitational lensing and the geometry of spacetime described by the Schwartzschild metric.

5. What are some real-life applications of the Schwartzschild metric and its image amplification predictions?

The Schwartzschild metric and its predictions about image amplification have been used in a variety of applications, including studying the effects of massive objects like black holes on light from distant galaxies, testing the predictions of general relativity, and even aiding in the search for new planets and exoplanets in distant star systems.

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