Distinguishing f(R) theories from general relativity by gravitational lensing effect
The post-Newtonian formulation of a general class of f ( R ) theories is set up in a third-order approximation. It turns out that the information of a specific form of f ( R ) gravity is encoded in the Yukawa potential, which is contained in the perturbative expansion of the metric components. Altho...
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Published in: | The European physical journal. C, Particles and fields Vol. 77; no. 11; pp. 1 - 9 |
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Main Authors: | , , , |
Format: | Journal Article |
Language: | English |
Published: |
Berlin/Heidelberg
Springer Berlin Heidelberg
01-11-2017
Springer Springer Verlag (Germany) SpringerOpen |
Subjects: | |
Online Access: | Get full text |
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Summary: | The post-Newtonian formulation of a general class of
f
(
R
) theories is set up in a third-order approximation. It turns out that the information of a specific form of
f
(
R
) gravity is encoded in the Yukawa potential, which is contained in the perturbative expansion of the metric components. Although the Yukawa potential is canceled in the second-order expression of the effective refraction index of light, detailed analysis shows that the difference of the lensing effect between the
f
(
R
) gravity and general relativity does appear at the third order when
f
′
′
(
0
)
/
f
′
(
0
)
is larger than the distance
d
0
to the gravitational source. However, the difference between these two kinds of theories will disappear in the axially symmetric spacetime region. Therefore only in very rare case the
f
(
R
) theories are distinguishable from general relativity by gravitational lensing effect in a third-order post-Newtonian approximation. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-017-5308-5 |