28.11.2012 Views

Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

162 EXACT SOLUTIONS AND SCALAR FIELDS IN GRAVITY<br />

(4). For this Bianchi mo<strong>de</strong>l it implies, by impos<strong>in</strong>g the condition that<br />

are constants, severe algebraic constra<strong>in</strong>ts on the scale factors, so it<br />

seems more likely that are functions. This expla<strong>in</strong>s why no totally<br />

anisotropic solution has been found yet. In Ref. [7] we<br />

have analyzed the case when the polynomial solution for is valid. In<br />

this case, unfortunately, we could not found explicitly the values of the<br />

constants If this solution is valid, however, one has that<br />

where D, F, G are constants. Accord<strong>in</strong>gly,<br />

Eq. (9) <strong>in</strong>dicates that the solution must tend, as time evolves, to the<br />

positive curvature FRW solution, i.e. one has aga<strong>in</strong> that as<br />

However, a <strong>de</strong>f<strong>in</strong>itive answer will arrive by obta<strong>in</strong><strong>in</strong>g explicitly<br />

the values of<br />

4. CONCLUSIONS<br />

We have presented a set of differential equations written <strong>in</strong> rescaled<br />

variables that are valid for Bianchi type I, V <strong>and</strong> IX mo<strong>de</strong>ls, as well as for<br />

FRW mo<strong>de</strong>ls with<strong>in</strong> general scalar–tensor theories, <strong>in</strong>clud<strong>in</strong>g Dehnen’s<br />

IG theory. It seems to be very difficult to solve analytically this system<br />

given by Eqs. (1), (4) <strong>and</strong> (6). However, for the special case <strong>in</strong> which the<br />

potential vanishes, or when matter terms dom<strong>in</strong>ate over the potential<br />

[9], that is for the BD case, one is able to f<strong>in</strong>d solutions. Accord<strong>in</strong>gly,<br />

one can <strong>in</strong>tegrate Eq. (10) for the cases of FRW mo<strong>de</strong>ls, <strong>and</strong> Bianchi<br />

type I <strong>and</strong> V mo<strong>de</strong>ls, because <strong>in</strong> these cases the anisotropic parameters<br />

are constants.<br />

The solutions discussed here are:<br />

(i) A particular solution for non-flat FRW mo<strong>de</strong>ls. We have found a<br />

new solution of Eq. (10) valid for curved FRW cosmologies, that<br />

is, a solution with This is the general solution subject to some<br />

constra<strong>in</strong>t that permits one to have two important physical cases: the<br />

case when hav<strong>in</strong>g some <strong>in</strong>terest <strong>in</strong> str<strong>in</strong>g cosmology [17], that<br />

implies an equation of state of a quasi dust mo<strong>de</strong>l <strong>and</strong> the case<br />

when consistent with current BD local experimental constra<strong>in</strong>ts<br />

[18], imply<strong>in</strong>g that The new solution is non-<strong>in</strong>flationary <strong>and</strong><br />

for asymptotic times is of power-law type.<br />

(ii) The general solution of Bianchi type I mo<strong>de</strong>l <strong>and</strong> a particular<br />

solution of type V; both solutions are quadratic polynomials. These<br />

solutions let the mo<strong>de</strong>ls isotropize as time evolves, however, this can<br />

happens only for some parameter range. The polynomial solution<br />

may also be valid for Bianchi type IX, but it is not proved yet. If it<br />

were, isotropization would be also guaranteed.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!