Strong gravitational lensing in f (x) = x3/2 gravity

被引:15
作者
Campigotto, M. C. [1 ,2 ]
Diaferio, A. [1 ,2 ]
Hernandez, X. [3 ]
Fatibene, L. [2 ,4 ]
机构
[1] Univ Torino, Dipartimento Fis, Via P Giuria 1, I-10125 Turin, Italy
[2] Ist Nazl Fis Nucl, Sez Torino, Via P Giuria 1, I-10125 Turin, Italy
[3] Univ Nacl Autonoma Mexico, Inst Astron, Mexico City 04510, DF, Mexico
[4] Univ Torino, Dipartimento Matemat, Via C Alberto 10, I-10123 Turin, Italy
来源
JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS | 2017年 / 06期
关键词
gravitational lensing; modified gravity; galaxy clusters; MODIFIED NEWTONIAN DYNAMICS; TULLY-FISHER RELATION; CLUSTER MASS; DARK-MATTER; MOND; GALAXIES; PROFILES; RAY;
D O I
10.1088/1475-7516/2017/06/057
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We discuss the phenomenology of gravitational lensing in the purely metric f (x) gravity, an f (R) gravity where the action of the gravitational field depends on the source mass. We focus on the strong lensing regime in galaxy-galaxy lens systems and in clusters of galaxies. By adopting point-like lenses and using an approximate metric solution accurate to second order of the velocity field vac, we show how, in the f (x) = x(3/2) gravity, the same light deflection can be produced by lenses with masses smaller than in General Relativity (GR); this mass difference increases with increasing impact parameter and decreasing lens mass. However, for sufficiently massive point-like lenses and small impact parameters, f (x) = x(3/2) and GR yield indistinguishable light deflection angles: this regime occurs both in observed galaxy-galaxy lens systems and in the central regions of galaxy clusters. In the former systems, the GR and f (x) masses are compatible with the mass of standard stellar populations and little or no dark matter, whereas, on the scales of the core of galaxy clusters, the presence of substantial dark matter is required by our point-like lenses both in GR and in our approximate f (x) = x(3/2) solution. We thus conclude that our approximate metric solution of f (x) = x(3/2) is unable to describe the observed phenomenology of the strong lensing regime without the aid of dark matter.
引用
收藏
页数:17
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