A&A 422, 831-839 (2004)
DOI: 10.1051/0004-6361:20035734
J. Cepa^{1,2}
1 - Instituto de Astrofísica de Canarias, 38200 La Laguna, Tenerife, Spain
2 -
Departamento de Astrofísica, Facultad de Física, Universidad de la Laguna,
38071 La Laguna, Tenerife, Spain
Received 24 November 2003 / Accepted 24 March 2004
Abstract
The currently available values and confidence limits for
, H_{0} and
globular cluster ages still indicate that the dark energy that dominates the Universe
could also be a form of quintessence or phantom energy. In fact, current cosmological values
favor phantom energy. To increase the likelihood of a cosmological constant as dark energy
instead of phantom energy, the possibilities seem to lie in reducing globular cluster ages,
the Hubble constant, or both, and possibly advancing the epoch of globular cluster formation.
For a set of possible dark energy equations of state that includes the cosmological constant,
quintessence or phantom energy, age-redshift analytical expressions for null curvature
universes that include ordinary matter are derived together with the corresponding ages
for these universes. "Cosmic coincidences'' are found for the currently accepted values of
when evaluating the age of the Universe with a cosmological constant
or a phantom energy as dark energies.
Key words: cosmology: theory - relativity - cosmology: cosmological parameters
Curvature, age, the Hubble constant and energy density form a long-standing cosmological puzzle. Measurements of the cosmic microwave background radiation (CMBR) anisotropy have confirmed that the Universe is consistent with null, or nearly null, curvature (de Bernardis et al. 2000), as predicted by the inflation paradigm. However, a Euclidean universe composed of ordinary matter only has an age inconsistent with that derived from globular clusters (Bolte & Hogan 1995). Moreover, galaxy cluster data (Carlberg et al. 1996) allow us to obtain only about 20-30% of the amount of matter required for achieving null curvature. This puzzle seemed to be solved by the discovery in 1998 of the first evidence for an accelerating universe based on distant type Ia Supernova (SNeIa) observations (Riess et al. 1998), which have been supported by additional data including more distant SNe (Riess et al. 2001). This acceleration implies the presence of a significant fraction of dark energy with an equation of state of negative pressure. The addition of the required amount of this energy to the observed amount of matter allows us to obtain the total amount of energy required for achieving null curvature. It also has the desired side effect of producing an older universe that can then be made consistent with independent age measurements.
However, the nature of this dark energy is still to be established. Moreover, its equation of state is still unknown. The first attempts rescued the cosmological constant as an ad hoc explanation, although their interpretation of the constant in terms of a vacuum energy is inconsistent by 124 orders of magnitude with respect to the required value, which leads us to assume that its value has to be zero for consistency. Other energy types, such as quintessence or phantom energy, have also been invoked, although their origin is no clearer than that of the cosmological constant.
Quintessences were introduced by Wetterich (1998), Caldwell et al. (1998), Ratra & Peebles (1998) to avoid the extreme fine-tuning needed to allow a cosmological constant to be significant only at recent epochs. Quintessences are characterized by a scalar field whose evolution depends on its potential. The most popular potentials are inverse power and exponential laws (Kneller & Strigari 2003 and references therein), although other possibilities have been considered (see, for example, Di Pietro & Claeskens 2003). Both inverse power laws and exponential potentials converge to a unique solution for a broad range of different initial conditions.
Phanton energy (Caldwell 1999) violates the dominant-energy condition (Hawking & Ellis 1973) that might allow the existence of wormholes. It also makes the Universe reach in a finite time a cosmic doomsday where all objects, from galaxies to nucleons, are ripped apart, a situation that has been termed the "big rip'' (Caldwell 1999). Although some Chaplygin gas model generalization can avoid this big rip (González-Díaz 2003), the violation of the dominant energy condition and the difficulties in obtaining a stable phantom model (Carroll et al. 2003) renders this kind of energy more problematic than quintessences.
In the case of either quintessences, the cosmological constant or phantom energy, it seems established that the introduction of negative pressure energies is required to fit and harmonize the existing CMBR anisotropy, SNeIa, clusters of galaxies, large scale structure, Big Bang nucleosynthesis and age estimator data.
The incorporation of these energies changes the age-redshift relation and estimates of the age of the Universe. The aim of this article is to show the difficulty in avoiding phantom energies with the current age estimator data and to provide analytical age expressions for the homogeneous and isotropic case for the most likely equations of state for our Universe, considered constant, as restricted by the cosmological parameters commonly assumed. These include the cosmological constant, quintessence and phantom energy.
Thomas & Kantowski (2000) provide an age-redshift relation using elliptical integrals for a universe composed of matter and a cosmological constant, but without providing an easy ready-to-use expression. In general, no analytical expressions of age as a function of redshift seems to be readily available in the literature for the currently most widely accepted cosmologies: flat universes of matter plus a cosmological constant, quintessence or phantom energy.
Although numerical integration allows us to obtain ages in a relatively straightforward way (see, for example, Hogg 2000), analytical solutions are faster to evaluate and have the advantage of providing more precise and ready results than numerical approaches. Moreover, analytical expressions provide the explicit dependence on energy densities, thereby easing their study. Finally, they constitute a reference for checking numerical solutions.
In Sect. 2 the basic equations are given. In Sect. 3 possible values for the equation of state, considered constant, are reviewed according to recent figures for the cosmological parameters, in Sect. 4 the general case of a non-constant equation of state is outlined, and in Sect. 5 analytical age-redshift relations and ages are obtained by solving the equations on a case by case basis for the range of the constant equations of state assumed.
The age-redshift relation can be obtained from the Friedmann equations. Using units
defined by c=G=1, where c is the speed of light and G the constant of gravitation,
the Friedmann equation representing energy balance can be written as
The total energy density as a function of redshift, z, is defined to be
This assumption, a generalization of the cosmological constant that represents a barotropic fluid, lacks physical justification. A constant w is valid for the cosmological constant only, since in general a time dependency is expected in quintessences and phantom energies. However, the absence of well motivated dark energy models based on fundamental physics and the difficulty to observe a time dependence of w either by using the CMBR (Aurich & Steiner 2003) or fits to luminosity distances (Di Pietro & Claeskens 2003), makes this assumption a reasonable model-independent approximation to the equation of state of these energies (see Kneller & Strigari 2003 and references therein for advantages and limitations of this approach). As a consequence, the constant w values inferred represent effectives values weighted with respect to (Doran et al. 2001; Doran & Lilley 2002). Nevertheless, a more general case is briefly outlined in Sect. 4.
For an
universe, then, the age-redshift relation can be obtained using
The age of the Universe, t_{0}, for a given combination of , and the Hubble constant, H_{0}, can be obtained by setting the lower limit of (3) to z=0.
Fits of observational data of good standard candles to distance-redshift relations can provide limits on the parameter w of the equation of state. The main limitations of this method comes from the uncertainties in the extinction and evolution of the selected candles and in the curvature, H_{0} and energy densities. Constraining the dark energy equation of state from the age of the Universe requires an accurate knowledge of H_{0}, , the curvature and t_{0}, where t_{0} is obtained from the age, , of globular cluster or halo stars used as age indicators, plus the time, , elapsed from the Big Bang to globular cluster formation. For this article, the following parameters have been assumed:
Figure 1: Universe age versus the equation of state of dark energy, w, for a null curvature universe with ordinary matter. The age becomes less sensitive to w as w decreases. | |
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Table 1: Upper limits for w obtained for the assumed values of and at 68% and 95% c.l. for globular cluster formation at z=3.
From the fit to distance-redshift relations using gravitational lenses and SN data, Waga & Miceli (1999) derive w<-0.7 (68% c.l.) and w<-0.6 (95.4% c.l.) for . Perlmutter et al. (1999) obtained w<-0.6 (95% c.l.) using SNeIa and large scale structure data. The age of the Universe was the procedure employed by Krauss & Chaboyer (2003) from globular cluster age estimates to obtain w<-0.7 (68% c.l.) and w<-0.45 (95% c.l.). A statistical analysis from WMAP (Wilkinson Microwave Anisotropy Probe) CMBR data combined with SNeIa and large scale structure data gives w<-0.78 at 95% c.l. (Spergel et al. 2003), with the previous w>-1. The results of Table 1 are then consistent with those obtained by other authors.
Although it is usually accepted that the most likely value that makes the existing data self-consistent is w=-1 (see, for example, Krauss & Chaboyer 2003; Spergel et al. 2003), the fact is that quintessence ( -1/3 > w > -1) cannot be ruled out on observational grounds using currently existing data. Moreover, the assumptions of this article do not allow us to rule out phantom energy (w<-1). In fact, the mean values assumed for , t_{0}, and give w=-4.95 for H_{0}=72 km s^{-1} kpc^{-1} and w=-1.49 for H_{0}=64 km s^{-1} kpc^{-1}. Taking into account that the w values inferred are effective values (Sect. 2), then w(t) must have been even smaller, which points strongly to an epoch of the Universe with w<-1.
An elementary analysis, varying only one of the parameters , , and H_{0} at a time, while keeping w=-1 fixed, gives the following results for the possible options to make the assumed mean values compatible with a cosmological constant instead of phantom energy:
Although obtaining a conclusive result, then, requires more accurate data on , H_{0}, and , there is prima facie qualitative evidence that the possibilities of reducing the current likelihood of phantom energy to favor a cosmological constant as dark energy reduces , H_{0} or both, and possibly advances the epoch of globular cluster formation.
Except in the case of the cosmological constant, energy densities vary with redshift. While non-relativistic matter and radiation can be represented by constant w, this do not generally happen with quintessences and phantom energies, although in these cases a constant w representing a weighted mean can be taken as an approximation.
As already stated in the introduction, quintessences were invoked to avoid the fine-tuning problem posed by the dominance of the cosmological constant in recent epochs only. Moreover, quintessences with w(z) might present some additional advantages such as string theory compatibility by avoiding the existence of an event horizon (Cline 2001). Many quintessence models that differ in the form of the potential have been proposed (see Doran et al. 2001 for some potentials used).
Phantom energies have been represented by González Díaz (2003) by means of a suitable generalization of the Chaplygin gas model.
In a general case, the differential equation governing the equation of state can be
derived from the Friedmann equations,
(4) |
With the hypotheses of null curvature and only two equations of state, one of them for
ordinary matter, (3) can be written as
Given the absence of widely accepted and physically indisputable dark energy models, a polynomial parameterization has been used by some authors as a simpler and pragmatic way to approximate the time dependence of the equation of state. The dependence so parameterized could then be fitted to different model predictions.
For example, Goliath et al. (2001) and Linder (2001) considered
linear models of the form
Although the age of the Universe cannot be used on its own to constrain two parameters, additional constraints may be invoked.
A strong constrain is that dark energies cannot dominate at high redshift. Otherwise, the expansion would be different and primordial nucleosynthesis would yield different helium abundances and the period of structure formation would be affected as well (Doran et al. 2001). This constraint may be formally represented by for , which gives, using Eqs. (5), (8) and (10), the conditions w_{1}<0 and w_{0}+w_{a}<0 for Eqs. (7) and (9), respectively. This strong constraint implies that for an equation of state of the form (7) phantom energies will necessarily be present at high redshift.
A weaker constraint, since it is not based on observational evidence, is that an event horizon should not be present since it poses problems for string theories. This is equivalent to a future non-accelerated universe. Formally, for . This condition gives, using Eqs. (5), (8) and (10), the conditions 1+3(w_{0}-w_{1})>0 and w_{a}>0 for Eqs. (7) and (9), respectively.
Figure 2: Possible pairs (w_{0}, w_{1}) defining a dark energy equation of state w(z)=w_{0}+w_{1}z that give an age of 12 and 13.4 Gyr corresponding to the minimum age of the Universe at 95% and 68% confidence levels, respectively. A null-curvature universe with ordinary matter, and 2 Gyr has been assumed. The regions w_{1}>0 and 1+3(w_{0}-w_{1})<0 define respectively the parameter space were dark energy becomes unacceptably high at high redshifts and an event horizon exists. | |
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Figure 3: Possible pairs (w_{0}, w_{a}) defining a dark energy equation of state w(z)=w_{0}+w_{a}z/(1+z) that give an age of 12 and 13.4 Gyr corresponding to the minimum age of the Universe at 95% and 68% confidence levels, respectively. A null-curvature universe with ordinary matter, and 2 Gyr has been assumed. The regions w_{0}+w_{a}>0 and w_{a}<0 define respectively the parameter space were dark energy becomes unacceptably high at high redshifts and an event horizon exists. | |
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Figures 2 and 3 show the pairs of values for w_{0} and w_{1} or w_{a}, for equations of state of the form (7) or (9), respectively, that give an age of the Universe compatible with the minimum values derived from globular clusters at 95% and 68% c.l., assuming that globular clusters were formed at z=3 in a flat universe with . The regions where dark energy densities grow unacceptably high at high redshifts are marked. In both cases long epochs where w<-1 are present, except for some w_{0}, w_{a} pairs corresponding to the lowest 98% c.l. age values (Fig. 3). Nominal age values produce even more negative w values. Hence, the conclusions of the previous section that favoring a cosmological constant as dark energy would probably require reducing , H_{0} or both, and possibly advancing the epoch of globular cluster formation, are reinforced.
The results of Table 1 show that the upper w limits range between -0.23 and -1.21. The first limit does not accelerate the Universe, since for this effect to happen w<-1/3 is required. Hence the most extreme upper limit for an accelerated universe may be taken as w=-1/3. The other extreme may be approximated by w=-4/3, since values of w=n/3, where n is an integer, make obtaining analytical solutions easier. Four null-curvature cases will therefore be considered: the quintessence limit w= -1/3, the quintessence w= -2/3, the cosmological constant w= -1 and the phantom energy w=-4/3. These should be considered as weighted mean approximations to w.
As can be deduced from Friedmann equations, this equation of state corresponds to a universe with
.
This is a non-accelerated universe corresponding to the limit between the decelerated
and accelerated cases. Integrating (3),
The integration of (3) give (Grössner & Hofreiter 1975):
(14) |
Equation (13) with
is then valid for epochs before the
coasting point. After the coasting point (as the present epoch would be were
our universe dominated by this quintessence), it is straightforward to
demonstrate that to the value of (13) for
twice
the value of the second term of (13) for
has to be
added. For example, for z=0 it is possible to obtain the age of this universe,
(16) |
The integration of (3) gives
Finally, for this equation of state, (17) can be rewritten to give
the evolution of the scale factor
Figure 4: Age-redshift relations in null-curvature universes with ordinary matter for each of the dark energy equations of state w considered and . | |
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Figure 5: Age of null-curvature universes with ordinary matter versus for each of the dark energy equations of state w considered. | |
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From the integration of (3) it is possible to obtain (Grössner
& Hofreiter 1975)
The value corresponds to the redshift at which the energy densities of dark and conventional matter are equal. The coasting point where is given by .
Again, Eq. (19) provides a good estimate for the age of the Universe when w=-4/3 for and .
Figure 4 gives the age-redshift relation for each equation of state for and . Figure 5 gives the age of the Universe for each equation of state versus . Table 2 gives the age of the Universe derived for each equation of state considered. Abramowitz & Stegun (1972) has been used for the evaluation of elliptical integrals.
Table 2: Values of H_{0}t_{0} for the different equations of state of dark energy and different for .
In the most accepted cosmological model the Universe is currently accelerated owing to a form of dark energy of unknown origin, as found via distance-redshift fits to high redshift SNeIa. This energy complements the fraction of ordinary matter so that the curvature is null, according to the observed CMBR anisotropy and the inflation paradigm. Also, the dark energy increases the age of the Universe for the same values of and H_{0} with respect to a universe composed of non-relativistic matter only, thus alleviating possible age conflicts.
In this article a recent determination of , t_{0} and H_{0} has been selected from the literature with the criterion of providing a set of cosmological parameters as model-independent as possible. A simple analysis shows that the weighted mean equation of state of dark energy has upper values in the range -0.23 > w > -1.21. Hence, not only a cosmological constant but also quintessence or phantom energy are also viable dark energy candidates from an observational point of view. In fact, the mean values of , t_{0} and H_{0} favor phantom energy over other alternatives. Moreover, a time-dependent w favors even more the existence of epochs with w<-1. It is qualitatively shown that to reduce the likelihood of phantom energy to favor a cosmological constant as dark energy, smaller globular cluster ages and/or smaller H_{0} values with respect to those currently determined are required. Pushing back globular cluster formation to earlier epochs cannot be ruled out, but only together with lower values of and/or H_{0}. Otherwise, an age conflict might still be present.
The range of upper w limits inferred is approximately covered by taking w=-n/3 for n=1,2,3,4. For each of these constant values of w, which include quintessence, the cosmological constant and phantom energy, analytical age-redshift solutions for Euclidean universes have been deduced and analytical age expressions derived. Some of these analytical solutions have not been derived before. Furthermore, no analytical expressions seem to be available in the literature for the range of the constant equations of state considered. Analytical equations are more precise, faster and readier to use than numerical calculations when evaluating the age of the Universe. Moreover, the explicit dependence on and renders their study easier. Finally, curious "cosmic coincidences'' make 1/H_{0} a good approximation for the age of the Universe for the currently accepted values assuming null curvature and a cosmological constant or a phantom energy as dark energies.
Acknowledgements
This work has been supported by the Spanish Plan Nacional de Astronomía y Astrofísica under grant AYA2002-01379. This research has made use of NASA's Astrophysics Data System.