scholarly journals Second order perturbations in the Randall-Sundrum infinite brane-world model

2001 ◽  
Vol 64 (8) ◽  
Author(s):  
Hideaki Kudoh ◽  
Takahiro Tanaka
Keyword(s):  
2007 ◽  
Vol 653 (2-4) ◽  
pp. 122-128 ◽  
Author(s):  
Sergio del Campo ◽  
Ramón Herrera

2015 ◽  
Vol 2015 ◽  
pp. 1-10
Author(s):  
A. Tofighi ◽  
M. Moazzen ◽  
A. Farokhtabar

In the generalized Randall-Sundrum warped brane-world model the cosmological constant induced on the visible brane can be positive or negative. In this paper we investigate profiles of vacuum expectation value of the bulk scalar field under general Dirichlet and Neumann boundary conditions in the generalized warped brane-world model. We show that the VEV profiles generally depend on the value of the brane cosmological constant. We find that the VEV profiles of the bulk scalar field for a visible brane with negative cosmological constant and positive tension are quite distinct from those of Randall-Sundrum model. In addition we show that the VEV profiles for a visible brane with large positive cosmological constant are also different from those of the Randall-Sundrum model. We also verify that Goldberger and Wise mechanism can work under nonzero Dirichlet boundary conditions in the generalized Randall-Sundrum model.


2001 ◽  
Vol 283 (1-2) ◽  
pp. 8-14 ◽  
Author(s):  
Matej Pavšič
Keyword(s):  

2009 ◽  
Vol 399 (4) ◽  
pp. 2079-2087 ◽  
Author(s):  
K. K. Nandi ◽  
A. I. Filippov ◽  
F. Rahaman ◽  
Saibal Ray ◽  
A. A. Usmani ◽  
...  

2008 ◽  
Vol 32 (11) ◽  
pp. 865-867
Author(s):  
Jia Bei ◽  
Li Xi-Guo ◽  
Zhang Peng-Ming

2003 ◽  
Vol 18 (15) ◽  
pp. 2703-2727 ◽  
Author(s):  
Y. M. CHO ◽  
I. P. NEUPANE

In the Randall–Sundrum (RS) brane-world model a singular delta-function source is matched by the second derivative of the warp factor. So one should take possible curvature corrections in the effective action of the RS models in the Gauss–Bonnet (GB) form. We present a linearized treatment of gravity in the RS brane-world with the Gauss–Bonnet modifications to Einstein gravity. We give explicit expressions for the Neumann propagator in arbitrary D dimensions and show that a bulk GB term gives, along with a tower of Kaluza–Klein modes in the bulk, a massless graviton on the brane, as in the standard RS model. Moreover, a nontrivial GB coupling can allow a new branch of solutions with finite Planck scale and no naked bulk singularity, which might be useful to avoid some of the previously known "no-go theorems" for RS brane-world compactifications.


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