共查询到20条相似文献,搜索用时 0 毫秒
1.
We argue that more cosmological solutions in massive gravity can be obtained if the metric tensor and the tensor Σμν defined by Stückelberg fields take the homogeneous and isotropic form.The standard cosmology with matter and radiation dominations in the past can be recovered and ΛCDM model is easily obtained.The dynamical evolution of the universe is modified at very early times. 相似文献
2.
A cosmological scenario with two branes (A and B) moving in a 5-dimensional bulk is considered. As in the case of ecpyrotic and born-again braneworld models it is possible that the branes collide. The energy-momentum tensor is taken to describe a perfect barotropic fluid on the A-brane and a phenomenological time-dependent cosmological constant on the B-brane. The A-brane is identified with our Universe and its cosmological evolution in the approximation of a homogeneous and isotropic brane is analysed. The dynamics of the radion (a scalar field on the brane) contains information about the proper distance between the branes. It is demonstrated that the deSitter type solutions are obtained for late time evolution of the braneworld and accelerative behaviour is anticipated at the present time. 相似文献
3.
Simon Davis 《General Relativity and Gravitation》2000,32(3):541-551
The quantum cosmology of a higher-derivative gravity theory arising from the heterotic string effective action is reviewed. A new type of Wheeler–DeWitt equation is obtained when the dilaton is coupled to the quadratic curvature terms. Techniques for solving the Wheeler–DeWitt equation with appropriate boundary conditions shall be described, and implications for semiclassical theories of inflationary cosmology will be outlined. 相似文献
4.
We summarize the approach to brane cosmology known as mirage cosmology and use it to determine the Friedmann equation on a 3-brane embedded in different bulk spacetimes all with one or more extra dimensions. Usually, when there is more than one extra dimension the junction conditions, central to the usual brane world scenarios, are difficult to apply. This problem does not arise in mirage cosmology because the brane is treated as a test particle in the background spacetime. We discuss in detail the dynamics of a brane embedded in two specific 10D bulk spacetimes, namely Sch-AdS5 × S5 and a rotating black hole, and from the dynamics—which are now rather more complicated since the brane can move in all the extra dimensions—determine the new dark fluid terms in the brane Friedmann equation. Some of these, such as the cosmological constant term, are seen to be bulk dependent. We then show explicitly how this mirage cosmology approach matches with the familiar junction condition approach when there is just one extra dimension. The issue of a varying speed of light in mirage cosmology is addressed and we find a scenario in which c
eff always increases, tending asymptotically to c
0 as the universe expands. Finally some comments are made regarding brane inflation and limitations of the mirage cosmology approach are also discussed. 相似文献
5.
6.
Relic abundance of asymmetric Dark Matter particles in brane world cosmological scenario is investigated in this article. Hubble expansion rate is enhanced in brane world cosmology and it affects the relic abundance of asymmetric Dark Matter particles. We analyze how the relic abundance of asymmetric Dark Matter is changed in this model. We show that in such kind of nonstandard cosmological scenario, indirect detection of asymmetric Dark Matter is possible if the cross section is small enough which let the anti-particle abundance kept in the same amount with the particle. We show the indirect detection signal constraints can be used to such model only when the cross section and the 5-dimensional Planck mass scale are in appropriate values. 相似文献
7.
J. P. Uzan 《International Journal of Theoretical Physics》2002,41(11):2299-2309
I review the main aspects of the simulated gravity that arises in brane-world models in which the reflection symmetry is broken. I recall its main aspects, show how a Newton-like force can be simulated on small scales, and discuss the post-Newtonian constraints as well as the cosmology of this model. 相似文献
8.
9.
We review how one can construct a deconstructed gravity by a transverse latticification of 5D General Relativity. The obtained theory is a multigravity theory, with link fields that are explicitly constructed out of the metric. We also discuss the spectrum of the theory at the level of the linearized
theory. 相似文献
10.
We use only the equation.of motion for an interacting system of gravity, dilaton and antisymmetric tensor to study the soliton solutions by making use of a Poincaré-invariant ansatz. We show that the system of equations is completely integrable and the solution is unique with appropriate boundary conditions. Some new classes of solutions are also given explicitly. 相似文献
11.
We present the complete explicit brane solution in D-dimensional coupled gravity system. 相似文献
12.
Rainer Dick 《General Relativity and Gravitation》2004,36(1):217-224
I reconsider the problem of the Newtonian limit in nonlinear gravity models in the light of recently proposed models
with inverse powers of R. Expansion around a maximally symmetric local background with curvature scalar R
0 > 0 gives the correct Newtonian limit on length scales R
0
–1/2 if the gravitational Lagrangian
satisfies f(R
0)f(R0) 1, and I propose two models with f(R
0) = 0. 相似文献
13.
PING Yong-Li XU Li-Xin CHANG Bao-Rong LIU Hong-Ya 《理论物理通讯》2008,50(8):383-386
Current universe (assumed here to be normal matter on the brahe) is pressureless from observations. In this case the energy condition is po ≥ 0 and po =O. By using this condition, brahe models can be distinguished. Then, assuming arbitrary component of matter in DGP model, we use four known energy conditions to study the matter on the brahe. If there is nonnormal matter or energy (for example dark energy with w 〈-1/3) on the brane, the universe is accelerated. 相似文献
14.
Inspired by the f(R) non-linear massive gravity,we propose a new kind of modified gravity model,namely f(T) non-linear massive gravity,by adding the dRGT mass term reformulated in the vierbein formalism,to the f(T)theory.We then investigate the cosmological evolution of f(T) massive gravity,and constrain it by using the latest observational data.We find that it slightly favors a crossing of the phantom divide line from the quintessence-like phase(ω_(de) -1) to the phantom-like one(ω_(de) -1) as redshift decreases. 相似文献
15.
In recent years an increasing number of papers have attempted to mimic or supplant quantum field theory in discussions of issues related to gravity by the tools and through the perspective of quantum information theory, often in the context of alternative quantum theories. In this article, we point out three common problems in such treatments. First, we show that the notion of interactions mediated by an information channel is not, in general, equivalent to the treatment of interactions by quantum field theory. When used to describe gravity, this notion may lead to inconsistencies with general relativity. Second, we point out that in general one cannot replace a quantum field by a classical stochastic field, or mock up the effects of quantum fluctuations by that of classical stochastic sources (noises), because in so doing important quantum features such as coherence and entanglement will be left out. Third, we explain how under specific conditions semi-classical and stochastic theories indeed can be formulated from their quantum origins and play a role at certain regimes of interest. 相似文献
16.
Hui-Qing Lu Li-Ming Shen Guo-Hong Yang Y. Y. Lai K. S. Cheng 《International Journal of Theoretical Physics》2002,41(5):939-951
We apply the theory developed in quantum cosmology to a model of charged generalized Brans–Dicke gravity. This is a quantum model of gravitation interacting with a charged Brans–Dicke type scalar field which is considered in the Pauli frame. The Wheeler–DeWitt equation describing the evolution of the quantum Universe is solved in the semiclassical approximation by applying the WKB approximation. The wave function of the Universe is also obtained by applying both the Vilenkin-like and the Hartle–Hawking-like boundary conditions. We then make predictions from the wave functions and infer that the Vilenkin's boundary condition is more reasonable in the Brans–Dicke gravity models leading a large vacuum energy density at the beginning of the inflation. 相似文献
17.
Current universe (assumed here to be normal matter on the brane) is
pressureless from observations. In this case the energy condition is
ρ0≥0 and p0=0. By using this condition, brane models can be distinguished. Then, assuming arbitrary component of matter in
DGP model, we use four known energy conditions to study the matter
on the brane. If there is nonnormal matter or energy (for example
dark energy with w<-1/3) on the brane, the universe is accelerated. 相似文献
18.
A cosmological model based on gauge theory of gravity is proposed in this paper. Combining cosmological principle
and field equation of gravitational gauge field, dynamical equations of the scale factor R(t) of our universe can be
obtained. This set of equations has three different solutions.
A prediction of the present model is that, if the energy density of the universe is not zero and the universe is
expanding, the universe must be space-flat, the total energy
density must be the critical density
ρc of the universe. For space-flat case, this model gives the same solution as that of the Friedmann model. In other words, though they have different dynamics of
gravitational interactions, general relativity and gauge
theory of gravity give the same cosmological model. 相似文献
19.
20.
S. Capozziello V. I. Man’ko G. Marmo C. Stornaiolo 《General Relativity and Gravitation》2008,40(12):2627-2647
The probability representation, in which cosmological quantum states are described by a standard positive probability distribution,
is constructed for minisuperspace models selected by Noether symmetries. In such a case, the tomographic probability distribution
provides the classical evolution for the models and can be considered an approach to select “observable” universes. Some specific
examples, derived from Extended Theories of Gravity, are worked out. We discuss also how to connect tomograms, symmetries
and cosmological parameters. 相似文献