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 $ \star $ The phenomenology of black energy: The new matter shape?

The theorists proposed many possibilities to account for black energy:

The simplest way of paramétriser this energy black is its equation of state.

As we saw the universe is homogeneous and isotropic this implies that the tensor energy impulse must take a form corresponding to a true fluid:

$\displaystyle T_X^{\mu \nu} = diag\left[ \rho_{X}, -P_X,-P_X,-P_X\right]$ (1.33)

where  $ \rho_X^{1/4 } = 2-3.10^{-3}eV$ .

One can characterize the pressure by his report/ratio with the density of energy:

$\displaystyle \omega_X \equiv \frac{P_X}{\rho_X}$ (1.34)

 $ \omega$ constant. We see that the values most favoured are between -0.7 and -1. This already seems to exclude the topological models of defects.


Table 1.2: Equation of state of black energy according to its nature. In the case of quintessence  $ \omega$ varies dynamically between -1 and 1.
X $ \omega_X$
Cosmological constant  $ \Lambda $ -1
cosmic strings -1/3
Walls of field -2/3
Quintessence $ \frac{1/2 \dot \phi^2 -V(\phi)}{1/2\dot \phi^2 + V(\phi)}$


Figure 1.9: Ellipse in the plan  $ (\omega, \Omega _ { \rm M})$ for a flat universe. In top, measurements are presented coming from the supernovæ. In the medium, are superimposed the ellipses of the supernovæ, that coming from measurement on the great structures by 2dF and that coming from the observation from the cosmological diffuse bottom. In bottom the combined limits of these three measurements are represented. This figure is drawn from knop2003.
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Julien Raux 2004-05-04