Eur. Phys. J. C (2015) 75:569
DOI 10.1140/epjc/s10052-015-3803-0
Regular Article - Theoretical Physics
Thick brane in f (R) gravity with Palatini dynamics
D. Bazeia
1,a
, L. Losano
1,b
, R. Menezes
2,3,c
, Gonzalo J. Olmo
1,4,d
, D. Rubiera-Garcia
1,5,6,e
1
Departamento de Física, Universidade Federal da Paraíba, João Pessoa, PB 58051-900, Brazil
2
Departamento de Ciências Exatas, Universidade Federal da Paraíba, Rio Tinto, PB 58297-000, Brazil
3
Departamento de Física, Universidade Federal de Campina Grande, Campina Grande, PB 58109-970, Brazil
4
Departamento de Física Teórica, IFIC, Centro Mixto Universidad de Valencia-CSIC, Universidad de Valencia, 46100 Burjassot, Valencia, Spain
5
Faculdade de Ciências, Instituto de Astrofísica e Ciências do Espaço, Universidade de Lisboa, Campo Grande, 1749-016 Lisbon, Portugal
6
Department of Physics, Center for Field Theory and Particle Physics, Fudan University, 220 Handan Road, Shanghai 200433, China
Received: 4 February 2015 / Accepted: 20 November 2015 / Published online: 30 November 2015
© The Author(s) 2015. This article is published with open access at Springerlink.com
Abstract This work deals with modified gravity in five-
dimensional space-time. We study a thick Palatini f (R)
brane, that is, a braneworld scenario described by an anti-
de Sitter warped geometry with a single extra dimension of
infinite extent, sourced by a real scalar field under the Palatini
approach, where the metric and the connection are regarded
as independent degrees of freedom. We consider a first-order
framework which we use to provide exact solutions for the
scalar field and warp factor. We also investigate a perturba-
tive scenario such that the Palatini approach is implemented
through a Lagrangian f (R) = R + R
n
, where the small
parameter controls the deviation from the standard thick
brane case. In both cases it is found that the warp factor
tends to localize the extra dimension due to the nonlinear
corrections.
1 Introduction
Investigations dealing with space-time engendering higher
spatial dimensions started in physics soon after the appear-
ance of general relativity (GR) through the Kaluza–Klein
models (see e.g. [1] for a review), aimed to study unification
of the electromagnetic interaction with gravity. Nowadays,
the presence of higher spatial dimensions is very natural in
high energy physics, in string, superstring and other unifica-
tion and fundamental theories [2,3]. However, the addition of
extra spatial dimensions is in conflict with the natural world
which, when probed in any experiment, has only revealed the
a
e-mail: bazeia@fisica.ufpb.br
b
e-mail: losano@fisica.ufpb.br
c
e-mail: rmenezes@dce.ufpb.br
d
e-mail: gonzalo.olmo@csic.es
e
e-mail: drgarcia@fc.ul.pt
presence of three spatial dimensions, though proposals using
large extra dimensions with potential experimental signatures
in particle accelerators have been discussed [4–7].
To reconcile the constraint of three spatial dimensions of
the natural world with the introduction of extra dimensions,
important scenarios have been proposed. Here we focus our
attention upon the Randall–Sundrum (RS) work [8], where
the relevant portion of the higher-dimensional space-time is
embedded within a five-dimensional anti-de Sitter (AdS
5
)
geometry. This scenario assumes that the (3, 1) space-time
that describes the natural world is embedded in an AdS
5
warped geometry, with a single extra spatial dimension of
infinite extent. This is known as the RS2 braneworld scenario,
and the warp factor identifies a thin brane profile, decaying
along the extra dimension y in the form exp(−2|y|).
Soon after the proposed thin braneworld scenario, it was
modified with the presence of scalar fields, giving rise to
a new, very interesting thick braneworld scenario, in which
the warp factor is now described by another function, which
depends on the specific scalar field model one considers [9–
12]. The presence of scalar fields brought interesting possi-
bilities, as the appearance of a new feature, the splitting of
the brane, which emerges in the presence of distinct effects,
at finite temperature [13] or with specific scalar field models
[14,15] in the presence of at least one additional parameter,
to be used to control the splitting of the brane.
Like the number of spatial dimensions, there are other
foundational aspects of the idea of gravitation as a geo-
metric phenomenon which are likely to provide interest-
ing new viewpoints on the fundamental open questions of
gravitational physics. In this sense, most extensions of GR
adopt the implicit assumption that space-time is a Rieman-
nian structure completely determined by the metric degrees
of freedom (see e.g. [16–19] for some reviews). However,
though geometry made its appearance in physics through
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