TY - JOUR
T1 - De Sitter thick brane solution in Weyl geometry
AU - Liu, Yu Xiao
AU - Yang, Ke
AU - Zhong, Yuan
PY - 2010
Y1 - 2010
N2 - In this paper, we consider a de Sitter thick brane model in a pure geometric Weyl integrable five-dimensional space-time, which is a generalization of Riemann geometry and is invariant under a so-called Weyl rescaling. We find a solution of this model via performing a conformal transformation to map the Weylian structure into a familiar Riemannian one with a conformal metric. The metric perturbations of the model are discussed. For gravitational perturbation, we get the effective modified Poschl-Teller potential in corresponding Schrodinger equation for Kaluza-Klein (KK) modes of the graviton. There is only one bound state, which is a normalizable massless zero mode and represents a stable 4-dimensional graviton. Furthermore, there exists a mass gap between the massless mode and continuous KK modes. We also find that the model is stable under the scalar perturbation in the metric. The correction to the Newtonian potential on the brane is proportional to e-3rβ/2/r2, where β is the de Sitter parameter of the brane. This is very different from the correction caused by a volcano-like effective potential.
AB - In this paper, we consider a de Sitter thick brane model in a pure geometric Weyl integrable five-dimensional space-time, which is a generalization of Riemann geometry and is invariant under a so-called Weyl rescaling. We find a solution of this model via performing a conformal transformation to map the Weylian structure into a familiar Riemannian one with a conformal metric. The metric perturbations of the model are discussed. For gravitational perturbation, we get the effective modified Poschl-Teller potential in corresponding Schrodinger equation for Kaluza-Klein (KK) modes of the graviton. There is only one bound state, which is a normalizable massless zero mode and represents a stable 4-dimensional graviton. Furthermore, there exists a mass gap between the massless mode and continuous KK modes. We also find that the model is stable under the scalar perturbation in the metric. The correction to the Newtonian potential on the brane is proportional to e-3rβ/2/r2, where β is the de Sitter parameter of the brane. This is very different from the correction caused by a volcano-like effective potential.
KW - Field theories in higher dimensions
KW - Large extra dimensions
UR - https://www.scopus.com/pages/publications/78649701831
U2 - 10.1007/JHEP10(2010)069
DO - 10.1007/JHEP10(2010)069
M3 - 文章
AN - SCOPUS:78649701831
SN - 1126-6708
VL - 2010
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 10
M1 - 69
ER -