2012
DOI: 10.1103/physrevd.86.044028
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Geodesic congruences and their deformations in Bertrand space-times

Abstract: We study the energy conditions and geodesic deformations in Bertrand space-times. We show that these can be thought of as interesting physical space-times in certain regions of the underlying parameter space, where the weak and strong energy conditions hold. We further compute the ESR parameters and analyze them numerically. The focusing of radial time-like and radial null geodesics is shown explicitly, which verifies the Raychaudhuri equation. *

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Cited by 4 publications
(14 citation statements)
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“…The fact that bigger galaxies have steeper rotational velocity curves, fits well with experimental data. 10 For n < 1, the flat region of the galactic rotation curve falls within the BST. Hence in our model, matching the galactic rotation curves will require a choice of n. In this paper, we only discuss the case n = 2.…”
Section: Introductionmentioning
confidence: 87%
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“…The fact that bigger galaxies have steeper rotational velocity curves, fits well with experimental data. 10 For n < 1, the flat region of the galactic rotation curve falls within the BST. Hence in our model, matching the galactic rotation curves will require a choice of n. In this paper, we only discuss the case n = 2.…”
Section: Introductionmentioning
confidence: 87%
“…If we demand that the matching condition of our solution does not have a thin shell at the boundary then M 0 = 1/5 and M = r b /5. If we choose a typical matching radius r b ∼ 20 kpc and then restore normal units, 11 we obtain M ∼ 10 17 M ⊙ , i.e the Schwarzschild mass of the interior region turns out to be four to five orders greater than the general mass range of heavy galaxies. If we assume matching with a thin shell at the boundary and take β = 10 −3 , i.e M 0 ∼ 1/2, the Schwarzschild mass does not change appreciably.…”
Section: Introductionmentioning
confidence: 92%
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“…(33), and energy conditions for BSTs of the form presented in Eq. (11) have been established in [20]. It is reasonable to demand that the matter contribution to the energy density of Eq.…”
Section: Bsts In the Metric F (R) Gravity Paradigmmentioning
confidence: 99%
“…Also ν = 2M/B, and in the limit ν → 1, i.e q = 0, the Schwarzschild metric is recovered. On the other hand, the general form of the energy-momentum tensor and their relationship with the energy density and principal pressures for BSTs are as follows [20] :…”
Section: Galactic Rotation Curves and Bstsmentioning
confidence: 99%