

Effect of the curvature of light rays, due to the intense solar gravitational field, on the positioning of a distant star. Credits: NASA.
Combining optics and general relativity
This phenomenon of light deflecting when passing through a gravitational field had been known since Newton’s time. Thinking of light as tiny projectiles, the German scientist Johan Georg von Soldner obtained a first result for the angle of deflection of starlight when it grazes the solar disk . He obtained an astonishing 0.87 arc seconds (i.e. an angle 372,414 times smaller than a right angle). It was not until the development of Einstein’s theory of general relativity that this value was doubled to the world-famous 1.75”. This result was confirmed experimentally by the British astronomer Arthur Eddington during his famous solar eclipse expeditions of 29 May 1919. That famous eclipse proved Einstein right and catapulted him to worldwide fame.
This NASA animation illustrates the effect of light rays bending as they approach an intense gravitational field such as that of the Sun. Credits: NASA, ESA, and Goddard Space Flight Center/K. Jackson.
Studying the mirage
Eddington claimed that the calculation could also be carried out (with a high degree of accuracy) in an alternative way, based on considerations of geometrical optics. In this way, the effect of the curvature of light rays could be explained on the basis of the well-known phenomenon of mirages, caused by the curvature of light rays (refraction) in layers of air of varying density.
Illustration of a mirage in the desert when the warmer layers of air (close to the surface) have a different refractive index than the upper (colder) layers. As a result, the paths of the light rays coming from the object (the camel’s head), which pass through the different layers of air, reach the observer describing a curved path. Credits: Encyclopedia Britannica.
The PPN method to make Einstein’s equations easier
The exact calculation of this angle is not an easy task, since it involves solving complex differential equations within the framework of Einsteinian general relativity. Approximate analytical solutions are often used based on the so-called post-Newtonian method (PPN) , which expresses Einstein’s complicated equations in terms of deviations from Newton’s law of universal gravitation up to different orders. This PPN approach is widely used in astronomy to correct the positions of distant stars. This is what the European Space Agency’s GAIA observatory does, for example, to provide a highly detailed map of the stars in the Milky Way. Our MMA calculation method accurately reproduces the angle of light deflection for a gravitational field like that of the Sun. And we find differences.
Discrepancy between the first-order PPN formalism and our new exact equation (optical MMA method) for the angle of light deflection, for solar system bodies (left panel) and extrasolar sources (right panel). The main light deflector is considered to be the Sun, with larger differences (in reddish-orange tones) for bodies in the asteroid belt.
A better description of the orbits of minor bodies
One potential application of this new development would be a better determination of the orbits of smaller bodies around the Sun, such as asteroids. Greater precision in their initial positioning will lead to better prediction of their orbit.
An example of the application of our new result to the precise localization of asteroids and minor bodies in the Solar System. The illustration shows the particular cases of the asteroid Apophis (left panel) and Dimorphos (right panel).
Proxima Centauri and its exoplanet
Moving away from the Solar System, our theoretical result would also be applicable to the precise positioning of the closest star to the Sun, Proxima Centauri , and the exoplanet orbiting it, Proxima Centauri b .
Artist’s impression of the exoplanet Proxima Centauri b. Credits: ESO/M. KORNMESSER.