ar X iv : g r - qc / 0 20 70 01 v 3 2 7 N ov 2 00 2 Variation of G , Λ ( 4 ) and Vacuum Energy From Brane - World Models

نویسنده

  • J. Ponce
چکیده

In brane-world theory in five dimensions, the bulk metric is usually written in gaussian coordinates, where g 4µ = 0 and g 44 = −1. However, the choice g 44 = −1 is an external condition, not a requirement of the field equations. In this paper we study the consequences of having g 44 = ǫΦ 2 , where ǫ = ±1 and Φ is a scalar function varying with time, ˙ Φ = 0. This varying field entails the possibility of variable fundamental physical " constants ". These variations are different from those predicted in scalar-tensor and multidimensional theories. We solve the five-dimensional equations for a fixed brane and use the brane-world paradigm to determine the fundamental parameters in the theory, which are the vacuum energy σ, the gravitational coupling G and the cosmological term Λ (4). We present specific models where these physical quantities are variable functions of time. Different scenarios are possible but we discuss with some detail a model for which ˙ G/G ∼ H and Λ (4) ∼ H 2 , which seems to be favored by observations. Our results are not in contradiction to previous ones in the literature. In particular, to those where the brane is described as a domain wall moving in a static Sch − AdS bulk. Indeed these latter models in RS scenarios describe the same spacetime as other solutions (with fixed brane) in gaussian coordinates with ˙ Φ = 0. We conclude that the introduction of a time-varying Φ in brane-world theory yields a number of models that show variation in the fundamental physical " constants " and exhibit reasonable physical properties.

برای دانلود رایگان متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

ar X iv : g r - qc / 0 20 70 01 v 2 1 7 N ov 2 00 2 Variation of G , Λ ( 4 ) and Vacuum Energy From Brane - World Models

In brane-world theory in five dimensions, the bulk metric is usually written in gaussian coordinates, where g 4µ = 0 and g 44 = −1. However, the choice g 44 = −1 is an external condition, not a requirement of the field equations. In this paper we study the consequences of having g 44 = ǫΦ 2 , where ǫ = ±1 and Φ is a scalar function varying with time, ˙ Φ = 0. This varying field entails the poss...

متن کامل

ar X iv : g r - qc / 0 20 70 01 v 1 2 9 Ju n 20 02 Variation of G , Λ ( 4 ) and Vacuum Energy From Brane - World Models

In brane-world theory in five dimensions, the bulk metric is usually written in gaussian coordinates, where g 4µ = 0 and g 44 = −1. However, the choice g 44 = −1 is not mandatory. The presence of matter in the brane can generate temporal and spatial variations of g 44 , which in turn backreact on the brane. In this paper we study the consequences of having g 44 = ǫΦ 2 , where ǫ = ±1 and Φ is a ...

متن کامل

ar X iv : g r - qc / 0 30 50 41 v 1 1 1 M ay 2 00 3 Brane - Universes with Variable G and Λ ( 4 )

We investigate the cosmological consequences of a brane-world theory which incorporates time variations in the gravitational coupling G and the cosmological term Λ (4). We analyze in detail the model where ˙ G/G ∼ H and Λ (4) ∼ H 2 , which seems to be favored by observations. We show that these conditions single out models with flat space sections. We determine the behavior of the expansion sca...

متن کامل

ar X iv : g r - qc / 0 21 20 45 v 2 5 J un 2 00 3 Does Cosmic No - Hair Conjecture in Brane Scenarios follow from General Relativity ?

In this paper we examine the Cosmic No-Hair Conjecture (CNHC) in brane world scenarios. For the validity of this conjecture, in addition to the strong and weak energy conditions for the matter field, a similar type of assumption is to be made on the quadratic correction term and there is a restriction on the non-local term. It is shown by examples with realistic fluid models that strong and wea...

متن کامل

ar X iv : g r - qc / 0 41 11 11 v 2 2 7 N ov 2 00 4 Anisotropic Brane Cosmology with Variable G and Λ

There are two fundamental physical parameters namely the gravitational coupling G and the cosmological term Λ, in the Einstein’s theory of general relativity. Usually these parameters are assumed to be constants. But recent experimental and (or) observational evidences suggest that it is not unlikely to have small variations [1] of these fundamental parameters. However, alternative ideas about ...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2002