Correspondence of F(R) gravity singularities in Jordan and Einstein frames

被引:81
作者
Bahamonde, Sebastian [1 ]
Odintsov, S. D. [2 ,3 ,4 ]
Oikonomou, V. K. [5 ,6 ]
Wright, Matthew [1 ]
机构
[1] UCL, Dept Math, Gower St, London WC1E 6BT, England
[2] IEEC CSIC, Inst Space Sci, C Can Magrans S-N, Barcelona 08193, Spain
[3] Passeig LluAs Co, ICREA, Barcelona 08010, Spain
[4] Kazan Fed Univ, Inst Phys, Dept Gen Rel Grav, Kazan 420008, Russia
[5] Tomsk State Univ Control Syst & Radioelect TUSUR, Lab Theoret Cosmol, Tomsk 634050, Russia
[6] Tomsk State Pedag Univ, Tomsk 634061, Russia
关键词
Modified gravity; Finite time singularities; Singular cosmology; Einstein-Jordan frame correspondence; SUDDEN FUTURE SINGULARITIES; DARK ENERGY; PHANTOM ENERGY; BIG RIP; COSMOLOGY; QUANTUM; PARAMETERS; EQUATION; UNIVERSE; MODELS;
D O I
10.1016/j.aop.2016.06.020
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We study the finite time singularity correspondence between the Jordan and Einstein frames for various F(R) gravity theories. Particularly we investigate the ordinary pure F(R) gravity case and the unimodular F(R) gravity cases, in the absence of any matter fluids. In the ordinary F(R) gravity cases, by using specific illustrative examples, we show that it is possible to have various correspondences of finite time singularities, and in some cases it is possible a singular cosmology in one frame might be non-singular in the other frame. In the unimodular F(R) gravity case, the unimodular constraint is affected by the conformal transformation, so this has an effect on the metric we choose. Moreover, we study the Einstein frame counterpart theory of the unimodular F(R) gravity case, and we investigate the correspondences of the singularities in the two theories by considering specific illustrative examples. Finally, a brief dynamical system analysis is performed for the vacuum unimodular F(R) gravity and we demonstrate how the dynamical system behaves near the future Big Rip singularity. (C) 2016 Elsevier Inc. All rights reserved.
引用
收藏
页码:96 / 114
页数:19
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