A new plane symmetric solution and its application in cosmology

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Presentation transcript:

A new plane symmetric solution and its application in cosmology 张宏升 上海师范大学 Ref: PLB663 (2008) 291; 670 (2009) 271; 671 (2009) 428; 679 (2009) 81; 700 (2011) 97

Outline Taub solution Generalized ADS as the source of Taub The third brane model 2019/10/9 USTC

Plane symmetry A metric which permits 3 Killing vectors: two for translations and one for rotation. For vacuum case, one can prove there exists the 4th Killing vector, as the Birkhoff theorem in spherical case. 2019/10/9 USTC

Taub solution 2019/10/9 USTC

Taub’s theorem A perfect fluid cannot bound a vacuum in a space with plane symmetry unless the boundary condition of the continuity of the derivatives of the metric tensor is violated. 2019/10/9 USTC

Dolgov and Khriplovich’s theorem Any singularity free source with reflective symmetry for plane symmetric vacuum space does not exist. A.D. Dolgov, I.B. Khriplovich, Gen. Relativ. Gravit. 21 (1989) 13. 2019/10/9 USTC

Penrose diagram 2019/10/9 USTC

A new plane symmetric solution sourced by a perfect fluid 2019/10/9 USTC

Stress tensor 2019/10/9 USTC

A simplified class 2019/10/9 USTC

Reduced cases a=0 Minkowski b=0 Anti-de Sitter It can be regarded as a generalization of ADS. Thus we call it GADS 2019/10/9 USTC

Match to vacuum space Pressure should vanish on the ground, while density can keep a non-zero number. 2019/10/9 USTC

Match to Taub Boundary conditions 1. The metric is continuous 2. The jump condition 2019/10/9 USTC

Conclusion This new plane solution is a proper source of Taub space. 2019/10/9 USTC

Geodesics Contraction of the tangent vector 2019/10/9 USTC

Geodesics along z-direction 3-velocity 2019/10/9 USTC

Example of global equivalence principle We can not differentiate gravity or acceleration field. Reparametrization of time can reach a “constant acceleration” in 1+3 language. 2019/10/9 USTC

Higher dimensional case 2019/10/9 USTC

Junction condition 2019/10/9 USTC

The background of Brane universe Type I: (A)dS, for example Randall-Sundrum Type II: Minkowski, for example DGP The necessary condition for Brane model: the background permits a maximal symmetric 3-space, which serves as our space. 2019/10/9 USTC

The third brane The brane in 5d Taub and GADS 2019/10/9 USTC

Taub and GADS bulk 2019/10/9 USTC

Moving brane in Taub and GADS bulk 2019/10/9 USTC

2019/10/9 USTC

GADS brane 2019/10/9 USTC

Density evolution 2019/10/9 USTC

Evolution of W_de 2019/10/9 USTC

Evolution of H 2019/10/9 USTC

Thank you for your attention! 2019/10/9 USTC