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在星系团中观察到的病毒质量和重子质量之间的差异导致了缺失质量问题。 为解决此问题,已调用了一个新的非重子物质场,即暗物质。 但是,迄今为止,还没有暗物质成分的可能成分。 通过修改远距离引力来解释缺失的质量问题,从而产生了各种模型。 当考虑嵌入到高维时空中的低维流形上的有效场论时,对重力的修饰就显得非常自然。 已经显示出在具有以有限距离分隔的两个较低维歧管的情况下,能够解决缺失的质量问题,这又决定了麸分离的运动学。 还描述了银河系旋转曲线的后果。
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Eur. Phys. J. C (2016) 76:648
DOI 10.1140/epjc/s10052-016-4512-z
Regular Article - Theoretical Physics
Kinematics of radion field: a possible source of dark matter
Sumanta Chakraborty
1,a
, Soumitra SenGupta
2,b
1
IUCAA, Post Bag 4, Ganeshkhind, Pune University Campus, Pune 411 007, India
2
Department of Theoretical Physics, Indian Association for the Cultivation of Science, Kolkata 700032, India
Received: 11 July 2016 / Accepted: 11 November 2016 / Published online: 25 November 2016
© The Author(s) 2016. This article is published with open access at Springerlink.com
Abstract The discrepancy between observed virial and
baryonic mass in galaxy clusters have lead to the missing
mass problem. To resolve this, a new, non-baryonic mat-
ter field, known as dark matter, has been invoked. However,
till date no possible constituents of the dark matter compo-
nents are known. This has led to various models, by modi-
fying gravity at large distances to explain the missing mass
problem. The modification to gravity appears very naturally
when effective field theory on a lower-dimensional mani-
fold, embedded in a higher-dimensional spacetime is con-
sidered. It has been shown that in a scenario with two lower-
dimensional manifolds separated by a finite distance is capa-
ble to address the missing mass problem, which in turn deter-
mines the kinematics of the brane separation. Consequences
for galactic rotation curves are also described.
1 Introduction
Recent astrophysical observations strongly suggest the exis-
tence of non-baryonic dark matter at the galactic as well
as extra-galactic scales (if the dark matter is baryonic in
nature, the third peak in the Cosmic Microwave Background
power spectrum would have been lower compared to the
observed height of the spectrum [1]). These observations can
be divided into two branches – (a) behavior of galactic rota-
tion curves and (b) mass discrepancy in clusters of galaxies
[2].
The first one, i.e., rotation curves of spiral galaxies, shows
clear evidence of problems associated with Newtonian and
general relativity prescriptions [2–4]. In these galaxies neu-
tral hydrogen clouds are observed much beyond the extent
of luminous baryonic matter. In a Newtonian description,
the equilibrium of these clouds moving in a circular orbit of
radius r is obtained through equality of centrifugal and grav-
a
e-mails: sumantac.physics@gmail.com; sumanta@iucaa.in
b
e-mail: tpssg@iacs.res.in
itational force. For cloud velocity v(r ), the centrifugal force
is given by v
2
/r and the gravitational force by GM(r)/r
2
,
where M(r) stands for total gravitational mass within radius
r. Equating these two will lead to the mass profile of the
galaxy: M(r) = rv
2
/G. This immediately posed serious
problem, for at large distances from the center of the galaxy,
the velocity remains nearly constant v ∼ 200 km/s, which
suggests that mass inside radius r should increase monotoni-
cally with r , even though at large distance very little luminous
matter can be detected [2–4].
The mass discrepancy of galaxy clusters also provides
direct hint for existence of dark matter. The mass of galaxy
clusters, which are the largest virialized structures in the uni-
verse, can be determined in two possible ways – (i) from
the knowledge about motion of the member galaxies one can
estimate the virial mass M
V
, second, (ii) estimating mass of
individual galaxies and then summing over them in order to
obtain total baryonic mass M. Almost without any exception
M
V
turns out to be much large compared to M, typically one
has M
V
/M ∼ 20 − 30 [2–4]. Recently, new methods have
been developed to determine the mass of galaxy clusters;
these are (i) dynamical analysis of hot X-ray emitting gas
[5] and (ii) gravitational lensing of background galaxies [6]
– these methods also lead to similar results. Thus dynamical
mass of galaxy clusters are always found to be in excess com-
pared to their visible or baryonic mass. This missing mass
issue can be explained through postulating that every galaxy
and galaxy cluster is embedded in a halo made up of dark mat-
ter. Thus the difference M
V
−M is originating from the mass
of the dark matter halo the galaxy cluster is embedded in.
The physical properties and possible candidates for dark
matter can be summarized as follows: dark matter is assumed
to be non-relativistic (hence cold and pressure-less), inter-
acting only through gravity. Among many others, the most
popular choice being weakly interacting massive particles.
Among different models, the one with sterile neutrinos (with
masses of several keV) has attracted much attention [7,8].
Despite some success it comes with its own limitations. In
123
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648 Page 2 of 13 Eur. Phys. J. C (2016) 76 :648
the sterile neutrino scenario the X-ray produced from their
decay can enhance production of molecular hydrogen and
thereby speeding up cooling of gas and early star formation
[9]. Even after a decade long experimental and observational
efforts no non-gravitational signature for the dark matter has
ever been found. Thus a priori the possibility of breaking
down of gravitational theories at galactic scale cannot be
excluded [10–17].
A possible and viable way to modify the behavior of grav-
ity in our four-dimensional spacetime is by introducing extra
spatial dimensions. The extra dimensions were first intro-
duced to explain the hierarchy problem (i.e., observed large
difference between the weak and Planck energy scales) [18–
20]. However, the initial works did not incorporate gravity,
but they used large extra dimensions (and hence a large vol-
ume factor) to reduce the Planck scale to TeV scale. The
introduction of gravity, i.e., warped extra dimensions, dras-
tically altered the situation. In [21] it was first shown that
an anti-de Sitter solution in higher-dimensional spacetime
(henceforth referred to as bulk) leads to exponential sup-
pression of the energy scales on the visible four-dimensional
embedded sub-manifold (called a brane) thereby solving the
hierarchy problem. Even though this scenario of a warped
geometry model solves the hierarchy problem, it also intro-
duces additional correction terms to the gravitational field
equations, leading to deviations from Einstein’s theory at
high energy, with interesting cosmological and black hole
physics applications [22–30]. This conclusion is not bound
to Einstein’s gravity alone but it holds in higher curvature
gravity theories
1
as well [29,30,38]. Since the gravitational
field equations get modified due to the introduction of extra
dimensions it is legitimate to ask whether it can solve the
problem of missing mass in galaxy clusters. Several works
in this direction exist and can explain the velocity profile of
galaxy clusters. However, they emerge through the following
setup:
• Obtaining effective gravitational field equations on a
lower-dimensional hypersurface, starting from the full
bulk spacetime, which involves additional contributions
from the bulk Weyl tensor. The bulk Weyl tensor in spher-
ically symmetric systems leads to a component behav-
ing as mass and is known as “dark mass” (we should
emphasize that this notion extends beyond Einstein’s
gravity and holds for any arbitrary dimensional reduction
1
In addition to the introduction of extra dimensions we could also mod-
ify the gravity theory without invoking ghosts, which uniquely fixes the
gravitational Lagrangian to be Lanczos–Lovelock Lagrangian. These
Lagrangians have special thermodynamic properties and also modify
the behavior of four-dimensional gravity [31–37]. However, in this work
we shall confine ourselves exclusively within the framework of Einstein
gravity and shall try to explain the missing mass problem from kine-
matics of the radion field.
[29,30,38]). It has been shown in [39] that the introduc-
tion of the “dark mass” term is capable to yield an effect
similar to the dark matter. Some related aspects were also
explored in [40–43], keeping the conclusions unchanged.
• In the second approach, the bulk spacetime is always
taken to be anti-de Sitter such that bulk Weyl tensor van-
ishes. Unlike the previous case, which required S
1
/Z
2
orbifold symmetry, arbitrary embedding has been con-
sidered in [44] following [45]. This again introduces
additional corrections to the gravitational field equations.
These additional correction terms in turn lead to the
observed virial mass for galaxy clusters.
However, all these approaches are valid for a single brane
system. In this work we generalize previous results for a two
brane system. This approach not only gives a handle on the
hierarchy problem at the level of Planck scale but is also
capable of explaining the missing mass problem at the scale
of galaxy clusters. Moreover, in this setup the additional cor-
rections will depend on the radion field (for a comprehensive
discussion see [26]), which represents the separation between
the two branes. Hence in our setup the missing mass problem
for galaxy clusters can also shed some light on the kinematics
of the separation between the two branes.
Further the same setup is also shown to explain the
observed rotation curves of galaxies as well. Hence both
problems associated with dark matter, namely the missing
mass problem for galaxy clusters and the rotation curves for
galaxies, can be explained by the two brane system intro-
duced in this work via the kinematics of the radion field.
The paper is organized as follows – in Sect. 2, after pro-
viding a brief review of the setup we have derived effec-
tive gravitational field equations on the visible brane which
will involve additional correction terms originating from the
radion field to modify the gravitational field equations. In
Sect. 3 we have explored the connection between the radion
field, dark matter, and the mass profile of galaxy clusters
using relativistic Boltzmann equations along with Sect. 4
describing possible applications. Then in Sect. 5 we have
discussed the effect of our model on the rotation curve of
galaxies while Sect. 6 deals with a few applications of our
result in various contexts. Finally, we conclude with a dis-
cussion of our results.
Throughout our analysis, we have set the fundamental
constant c to unity. All the Greek indices μ, ν, α, . . . run
over the brane coordinates. We will also use the standard
signature (−++···) for the spacetime metric.
2 Effective gravitational field equations on the brane
The most promising candidate for getting effective gravita-
tional field equations on the brane originates from the Gauss–
123
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Eur. Phys. J. C (2016) 76 :648 Page 3 of 13 648
Codazzi equation. However, these equations are valid on a
lower-dimensional hypersurface (i.e., on the brane) embed-
ded in a higher-dimensional bulk. Hence this works only for
a single brane system. But the brane world model, addressing
the hierarchy problem, requires the existence of two branes,
where the above method is not applicable. To tackle the prob-
lem of a two brane system we need to invoke the radion field
(i.e., the separation between two branes), which has signif-
icant role in the effective gravitational field equations. The
bulk metric ansatz incorporating the above features takes the
following form:
ds
2
= e
2φ(y,x )
dy
2
+ q
μν
(y, x)dx
μ
dx
ν
. (1)
The positive and negative tension branes are located at
y = 0 and y = y
0
, respectively, such that the proper
distance between the two branes being given by d
0
(x) =
y
0
0
dy exp φ(x, y) and q
μν
stands for the induced met-
ric on y = constant hypersurfaces. The effective field
equations on the brane depend on the extrinsic curvature,
K
μν
= (1/2)£
n
q
μν
, where the normal to the surface is
n = exp(−φ)∂
y
but it also inherits a non-local bulk con-
tribution through E
μν
=
(5)
C
μανβ
n
α
n
β
,
(5)
C
μανβ
being
the bulk Weyl tensor. At first glance it seems that due to
non-local bulk effects the effective field equations cannot be
solved in closed form, but, as we will briefly describe, it
can be achieved through radion dynamics and at low energy
scales [46].
We will now proceed to derive low energy gravitational
field equations. As we have already stressed, unless one
solves for the non-local effects from the bulk the system of
equations would not close. Further it will be assumed that
curvature scale on the brane, L, is much larger than that
of bulk, . Then we can expand all the relevant geometri-
cal quantities in terms of the small, dimensionless parameter
= (/L)
2
. At zeroth order of this expansion, one recovers
(0)
q
μν
(y, x) = h
μν
(x) exp(−2d(y, x)/), while at the first
order one has [46]
(4)
G
μ
ν
=−
2
(1)
K
μ
ν
− δ
μ
ν
(1)
K
−
(1)
E
μ
ν
, (2)
e
−φ
∂
(1)
y
E
μν
=
2
(1)
E
μν
, (3)
e
−φ
∂
(1)
y
K
μ
ν
=−
D
μ
D
ν
φ+D
μ
φ D
ν
φ
+
2
(1)
K
μ
ν
−
(1)
E
μ
ν
.
(4)
The evolution equations for
(1)
E
μ
ν
and
(1)
K
μ
ν
can be solved,
(1)
E
μ
ν
= exp(4d(y, x)/)ˆe
μ
ν
(x), (5)
(1)
K
μ
ν
(y, x) = exp(2d(y, x)/)
(1)
K
μ
ν
(0, x )
−
2
1 − exp(−2d(y, x)/)
(1)
E
μ
ν
(y, x)
−
D
μ
D
ν
d(y, x) −
1
D
μ
dD
ν
d −
1
2
δ
μ
ν
(Dd )
2
,
(6)
where ˆe
μ
ν
= h
μα
e
αν
(x), with e
αν
(x) being the integration
constant of Eq. (3), which can be fixed using the junction
conditions [46],
2
1 − exp(−2d
0
/)
exp(4d
0
/)ˆe
μ
ν
(x)
=−
κ
2
2
exp(2d
0
/)T
(hid)μ
ν
+ T
(vis)μ
ν
−
D
μ
D
ν
d
0
− δ
μ
ν
D
2
d
0
+
1
D
μ
d
0
D
ν
d
0
+
1
2
δ
μ
ν
(Dd
0
)
2
(7)
where κ
2
stands for the bulk gravitational constant, T
(hid)μ
ν
stands for energy-momentum tensor on the hidden (positive
tension) brane, and T
(vis)μ
ν
for the visible (negative tension)
brane, respectively. Use of the expressions for
(1)
E
μ
ν
and
(1)
K
μ
ν
in Eq. (2) leads to the effective field equations on the
visible brane (i.e., the brane on which the Planck scale is
exponentially suppressed) in this scenario as [46]
(4)
G
μ
ν
=
κ
2
1
T
(vis)μ
ν
+
κ
2
(
1 +
)
2
T
(hid)μ
ν
+
1
D
μ
D
ν
− δ
μ
ν
D
2
+
ω()
2
D
μ
D
ν
−
1
2
δ
μ
ν
(
D
)
2
(8)
where the scalar field (x) appearing in the above effective
equation is directly connected to the radion field d
0
(x) (rep-
resenting the proper distance between the branes) such that
ω() and obey the following expressions [46]:
= exp
2d
0
− 1; ω() =−
3
2
1 +
. (9)
We will assume d
0
(x), the brane separation to be finite
and everywhere non-zero. This suggests that (x) should
always be greater than zero and shall never diverge. Finally
we also have a differential equation satisfied by from the
trace of Eq. (7), which can be written as [46]
D
μ
D
μ
=
κ
2
1
2ω + 3
T
(vis)
+ T
(hid)
−
1
2ω + 3
dω
d
D
μ
D
μ
(10)
123
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