Virbhadra–Ellis lens equation

The Virbhadra-Ellis lens equation [1] in astronomy and mathematics relates to the angular positions of an unlensed source ( β ) {\displaystyle \left(\beta \right)} , the image ( θ ) {\displaystyle \left(\theta \right)} , the Einstein bending angle of light ( α ^ ) {\displaystyle ({\hat {\alpha }})} , and the angular diameter lens-source ( D d s ) {\displaystyle \left(D_{ds}\right)} and observer-source ( D s ) {\displaystyle \left(D_{s}\right)} distances.

tan β = tan θ D d s D s [ tan θ + tan ( α ^ θ ) ] {\displaystyle \tan \beta =\tan \theta -{\frac {D_{ds}}{D_{s}}}\left[\tan \theta +\tan \left({\hat {\alpha }}-\theta \right)\right]} .

This approximate lens equation is useful for studying the gravitational lens in strong and weak gravitational fields when the angular source position is small.

References

  1. ^ Virbhadra, K. S.; Ellis, George F. R. (2000-09-08). "Schwarzschild black hole lensing". Physical Review D. 62 (8). American Physical Society (APS): 084003. arXiv:astro-ph/9904193. Bibcode:2000PhRvD..62h4003V. doi:10.1103/physrevd.62.084003. ISSN 0556-2821. S2CID 15956589.


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