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Strong field limit analysis of gravitational retro-lensing
General Relativity and Quantum Cosmology · Submitted 4 Nov 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We present a complete treatment in the strong field limit of gravitational retro-lensing by a static spherically symmetric compact object having a photon sphere.
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The abstract, sentence by sentence
We present a complete treatment in the strong field limit of gravitational retro-lensing by a static spherically symmetric compact object having a photon sphere. The results are compared with those corresponding to ordinary lensing in similar strong field situations. As examples of application of the formalism, a supermassive black hole at the galactic center and a stellar mass black hole in the galactic halo are studied as retro-lenses, in both cases using the Schwarzschild and Reissner-Nordstrom geometries.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a complete treatment in the strong field limit of gravitational retro-lensing by a static spherically symmetric compact object having a photon sphere. | contribution 1.00 | 0.94 | 0.20 | asserted 0.99 |
| s1 | The results are compared with those corresponding to ordinary lensing in similar strong field situations. | method 0.53 | 0.71 | 0.07 | asserted 0.88 |
| s2 | As examples of application of the formalism, a supermassive black hole at the galactic center and a stellar mass black hole in the galactic halo are studied as retro-lenses, in both cases using the Schwarzschild and Reissner-Nordstrom geometries. | contribution 0.81 | 0.89 | 0.08 | asserted 0.98 |
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The paper
Original abstract
We present a complete treatment in the strong field limit of gravitational retro-lensing by a static spherically symmetric compact object having a photon sphere. The results are compared with those corresponding to ordinary lensing in similar strong field situations. As examples of application of the formalism, a supermassive black hole at the galactic center and a stellar mass black hole in the galactic halo are studied as retro-lenses, in both cases using the Schwarzschild and Reissner-Nordstrom geometries.
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References
How the literature uses it
12 arXiv papers cite this in 15 sentences
Papers citing it · 7 sentences without a confident label
Uses its method or tool 1 paper
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Therefore, we attempt to approximate the apparent angle as was done in Refs. [ref] .
Gravitational lensing of massive particles in Reissner-Nordstr\"om spacetime · Lightlike ray lensing · 0.93
Compares with it 1 paper
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However, as expected, the lensing potential derived above, gives rise to a deflection angle, which in the geometric optics regime, matches with the weak field limit of the strong field calculations presented in [ref] (see Appendix [ref]).
Probing charge of compact objects with gravitational microlensing of gravitational waves · Lensing magnification by a charged black hole · 0.99
Cites it as background 5 papers
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In astrophysics, the rings with $n ≥1$ are often called photon rings [ref] , or the rings with $n=1$ and $n ≥2$ are called that $n=1$ photon ring and higher-order photon rings [ref] , respectively[ In gravitational lensing in a strong gravitational field, retrolensing images ($n=1$) [ref] and relativistic images ($n=2$) [ref] are also used.].
Constraints on the black-hole charges of M87* and Sagittarius A* by changing rates of photon spheres can be relaxed · Introduction · 0.84
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Strong deflection lensings by static and symmetric black holes [ref] and rotating black holes [ref] are widely studied and they can be used to discriminate black holes [ref] , naked singularities [ref] and wormholes [ref] as well as test gravity [ref] and its fundamental interaction with electromagnetic field [ref] .
Weak and strong deflection gravitational lensings by a charged Horndeski black hole · Introduction · 0.88
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Plenty works have done on the strong field lensings by a Schwarzchild black hole [ref] , by static and spherically symmetric spacetimes [ref] , by a Kerr black hole [ref] and by a Kerr black hole in the presence of the cosmological constant [ref] and electrically charge [ref] .
Strong field gravitational lensing by a charged Galileon black hole · Introduction · 0.97
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