Issue 
A&A
Volume 521, October 2010



Article Number  A52  
Number of page(s)  4  
Section  Cosmology (including clusters of galaxies)  
DOI  https://doi.org/10.1051/00046361/201014602  
Published online  20 October 2010 
BransDicke model constrained from the Big Bang nucleosynthesis and magnitude redshift relations of supernovae
(Research Note)
E. P. B. A. Thushari^{1}  R. Nakamura^{1}  M. Hashimoto^{1}  K. Arai^{2}
1  Department of Physics, Kyushu University, Fukuoka, 8128581, Japan
2 
Department of Physics, Kumamoto University, Kumamoto, 8608555, Japan
Received 31 March 2010 / Accepted 12 July 2010
Abstract
We investigated the BransDicke model with a variable cosmological term ()
with the coupling constant
.
We constrained the parameters inherent in this model from a comparison
between the Big Bang nucleosynthesis and the observed abundances.
Furthermore, we studied the magnitude redshift (mz) relations for the
with and without another constant cosmological term in a flat universe.
Observational data of type Ia supernovae (SNIa) are used in the
redshift range of 0.01<z<2.
We found that our model with an energy density of the constant
cosmological term of 0.7 can explain the SNIa observations, though
the model parameters are insensitive to the mz relation.
Key words: primordial nucleosynthesis  dark energy  early Universe  cosmology: observations  dark matter  cosmology: theory
1 Introduction
Astronomical observations indicate that the cosmological constant in the very early universe exceeds the present value by some 120 orders of magnitude, which is estimated in modern theories of elementary particles (Weinberg 1989). This is one of the finetuning problems in cosmology called the ``cosmological constant problem''. To explain the puzzle in cosmology, new modified theories are needed beyond the standard model. The behavior of the cosmological term has motivated various functional forms of the cosmological term. The mechanism of the dynamical reduction of the cosmological term is formulated as a time dependent function (Silviera & Waga 1997) and in terms of a scalar field (Weinberg 1989; Huterer & Turner 1999). On the other hand, generalized scalar tensor theories have been investigated (Wagoner 1970; Endo & Fukui 1977; Fukui et al. 2001).
One of them the BransDicke (BD) theory with a variable cosmological term () as a function of scalar field () (Endo & Fukui 1977). This model has been investigated for the early universe and constrained from the Big Bang nucleosynthesis (BBN) (Arai et al. 1987; Etoh et al. 1997; Nakamura et al. 2006) for the coupling constant . Present observations suggest that the value of exceeds 40 000 (Berti et al. 2003; Bertotti et al. 2005). Therefore it is worthwhile to reconstrain the parameters in the BransDicke model with a variable cosmological term () for a new value of . The has played a very important role in explaining the characteristics of the early universe (Arai et al. 1987; Etoh et al. 1997; Nakamura et al. 2006). However, we still need an answer to the question ``How does this model work at the present epoch?''. Therefore we adopt the magnitude redshift (mz) relations of type Ia supernova (SNIa) observations. This is because the cosmological term significantly affects the cosmic expansion rate of the universe at the low redshifts. The SNIa observations imply that the universe is accelerating at the present epoch (Perlmutter et al. 1999; Riess et al. 1998, 1999).
In Sect. 2 the formulation of the is reviewed. Parameters inherent in this model are constrained in Sect. 3 from the Big Bang nucleosynthesis for . In Sect. 4 the mz relation is investigated for the with including another constant cosmological term in a flat universe. Recent SNIa observational data (Astier et al. 2006; Riess et al. 2007; Kessler et al. 2009) are adopted to constrain the models. Concluding remarks are given in Sect. 5.
2 BransDicke model with a variable cosmological term
The field equations for the
are written as follows (Arai et al. 1987):
where is the scalar field and is the energymomentum tensor of the matter field. The RobertsonWalker metric for homogeneous and isotropic universe writes as (Weinberg 1972):
where a(t) is the scale factor and k is the curvature constant. Here we adopt c=1. The expansion is described by the following equation derived from the (0,0) component of Eq. (1):
where is the energy density.
We adopt the simplest case of the coupling between the scalar, and the matter field is
where is a constant. Assuming a perfect fluid for , Eq. (5) reduces to
where p is the pressure.
A particular solution of Eq. (2) is obtained from Eqs. (1) and (5):
where is the matter density at the present epoch.
The gravitational ``constant'' G is expressed as
The density and the pressure p are replaced by
where the energy density of matter varies as . The energy density of radiation is written as except epoch: at , where subscripts rad, and are for photons, neutrinos, and electronpositrons, respectively (Nakamura et al. 2006). The subscript ``0'' indicates the values at the present epoch.
Then, Eq. (6) is integrated to give
where B is an integral constant, and here we use the normalized value of B: .
Figure 1: Time evolutions of the scale factor in the with which are compared to the Friedmann model. 

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The original BransDicke theory is deduced for and is reduced to the Friedmann model when = const. and . Physical parameters have been used to solve Eqs. (4), (7), and (11): G_{0} = 6.6726 , (Spergel et al. 2003), and (Berti et al. 2003; Bertotti et al. 2005). Figure 1 shows the evolution of the scale factor in the for the several values of B^{*}. We identify considerable deviations in the from the Friedmann model at t<100 s, which depends on the specific parameters. Therefore the should be constrained from the BBN (Arai et al. 1987; Etoh et al. 1997; Nakamura et al. 2006).
3 Parameters constrained from the Big Bang nucleosynthesis
The Big Bang nucleosynthesis provides powerful constraints on possible deviation from the standard cosmology (Malaney & Mathews. 1993). As shown in Fig. 1, the expansion rates of the differ significantly from those of the standard Friedmann model.
The abundance of light elements in the has already been investigated (Arai et al. 1987; Etoh et al. 1997; Nakamura et al. 2006). In the previous studies, the parameters inherent in the have been constrained for . But we consider the case for convenience, because the Cassini measurements of the Shapiro time delay indicate 10^{4} (Berti et al. 2003; Bertotti et al. 2005). The detailed method of nucleosynthesis is described in Nakamura et al. 2006.
Figure 2 shows the calculated abundances of , , and for B^{*}=2 and . The uncertainties in nuclear reaction rates are indicated by the dashed lines. The horizontal dotted lines indicate the observational values of , , and as follows: Y_{p} = 0.2516 0.0080 (Fukugita & Kawasaki 2006; Carr et al. 2010), Y_{p}= 0.326 0.075 (Komatsu et al. 2010), 10^{5} (Pettini et al. 2008), 10^{10} (Melendez & Ramirez 2004). Here two observational values of are used. The solid vertical lines indicate the WMAP constraint of the baryontophoton ratio, 10^{10} (Komatsu et al. 2010).
The intersection range of the two observational values of is used to constrain the parameters. We found that the values of derived from and are tightly consistent with the value by the WMAP, though the lower limit of is barely consistent. These agreements lead us to obtain the parameter ranges of and .
Figure 2: Light element abundances of , , and vs. for B^{*}=2, , and . Dashed lines indicate the uncertainties in nuclear reaction rates in each abundance. The horizontal dotted lines indicate the regions of observational abundances. The solid vertical lines indicate the baryontophoton ratio . 

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4 m  z relation in the BD with and without a constant cosmological term
The distance modulus
of the source at the redshift z is
where m and M, are the apparent and absolute magnitudes respectively, and r_{l} stands for the radial distance in units of Mpc.
We adopt the SNIa (Astier et al. 2006; Riess et al. 2007; Kessler et al. 2009) for which
is defined by
where is given by Eq. (12), and are the observed values of distance modulus and their uncertinities.
For the homogeneous and isotropic universe, the relation between the
radial distance and the redshift is derived from the RobertsonWalker
metric as (Weinberg 2008)
where is the expansion rate written from Eq. (4) as
We conclude from the WMAP results that we live in a closely geometrically flat universe (Dunckley et al. 2009). The present matter density is obtained from Eq. (4) as
where the is the critical density of .
Using the analogy with the Lemaître model, Eq. (15) is transformed as
Here, the energy density parameters are defined as
The value is found to be very low as 7.01 10^{5} for . If we consider the absolute value of in the parameter range , its contribution to Eq. (17) is always less than 10^{5}. Therefore, as long as we consider the present epoch, contribution from can be neglected.
Figure 3: Distance modulus vs. redshift for the flat universe in the Friedmann model and the with and without constant cosmological term constrained by the SNIa observations (Riess et al. 2007; Astier et al. 2006; Kessler et al. 2009). 

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Figure 3 shows the mz relation in the for the SNIa observations. Matter is dominant in this model. The energy density of the cosmological term is always less than in the bestfit parameter region predicted in Sect. 3. The energy density of the cosmological term always takes negative values in the obtained parameter region. The parameter B^{*} is not effective to change the values of and . Because this model is matter dominant, it cannot be constrained by the SNIa observations.
The Friedmann model with the energy density parameters of is merged into the model with the reduced (where and N is defined as degrees of freedom). This is inconsistent with the present accelerating universe, which should contain a sufficient amount of dark energy to accelerate the universe. To explain the present accelerating universe, we need some modification of the cosmological term.
As the next approach, the
is modified by adding another constant cosmological term
.
The expansion rate in this model is written by
The present matter density is
Here the energy density parameter of the constant cosmological term is fixed to be 0.7.
We find that this model is consistent with the SNIa observations as seen in Fig. 3. The total cosmological term becomes large in this model and consistent with the present accelerating universe with reduced (where ). For , the with predicts 10^{2} and . always gets negative values in the parameter region of predicted in Sect. 3. If we consider the total value of energy densities, the contribution from to the total energy density is always between . Therefore the cosmological term is dominant in the present epoch and can be constrained from the present SNIa observations. We conclude that the with has nearly the same energy density parameters as the Friedmann model with . Although the cosmological term is not important at the early epoch, it plays a very important role at the present era. All the parameters inherent in the become insufficient as far as the mz relation is concerned.
5 Concluding remarks
Previous BBN calculations restricted the parameter range as  and  for (Nakamura et al. 2006). On the other hand, our high value of leads to reduces the parameter range of B^{*} ( ) and ( ). The models parameters are inefficient in the mz relations of the SNIa.
In Sect. 4, the value of is found to be much smaller compared with the other terms in Eq. (17). Even though is increased until 10^{4}, the contribution from to Eq. (17) is always less than in that particular parameter range. There is no considerably negative effect from the assumption we made in Sect. 4 to neglect the value of . In the parameter range , has taken negative values according to Eq. (17). This may not conflict with theories, because the pressure of dark energy must be negative to reproduce the present accelerated expansion (Carroll 1992).
Note that from Eq. (7), and at the present epoch, is directly connected with . Dark energy is written in terms of dark matter. However, dark energy and dark matter should be distinguishable to give rise to an accelerated expansion, because the evolution of the scale factor criticallydepends on the composition of each energy density of the universe. Therefore, the without a constant cosmological term is indistinguishable from the matterdominant Friedmann model with the parameters of . Note that the variable term in the plays a minor role to accelerate the universe at the present epoch. Because of this, we modified by adding a constant cosmological term. It has no relation to the expansion rate of the universe at the early epoch. However, the energy stored in the constant cosmological term played a major role in accelerating the universe at the present epoch as seen in Fig. 3. Since this model contains enough dark energy to accelerate the universe, it is constrained by the SNIa observations. In the present research, we investigated the at the early epoch to determine the intrinsic parameters and introduce new parameters at the present epoch for the mz relation. Because we demonstrated a possibility of a nonstandard model which is compatible with the observations, it is worthwhile to examine more generally the functional form of the cosmological term (e.g. Fukui et al. 2001).
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All Figures
Figure 1: Time evolutions of the scale factor in the with which are compared to the Friedmann model. 

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In the text 
Figure 2: Light element abundances of , , and vs. for B^{*}=2, , and . Dashed lines indicate the uncertainties in nuclear reaction rates in each abundance. The horizontal dotted lines indicate the regions of observational abundances. The solid vertical lines indicate the baryontophoton ratio . 

Open with DEXTER  
In the text 
Figure 3: Distance modulus vs. redshift for the flat universe in the Friedmann model and the with and without constant cosmological term constrained by the SNIa observations (Riess et al. 2007; Astier et al. 2006; Kessler et al. 2009). 

Open with DEXTER  
In the text 
Copyright ESO 2010
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