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

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New solutions of Bianchi mo<strong>de</strong>ls <strong>in</strong> scalar-tensor theories 157<br />

where <strong>and</strong> a column sum is given by where<br />

V or IX <strong>and</strong><br />

For the Bianchi type V mo<strong>de</strong>l one has the additional constra<strong>in</strong>t:<br />

imply<strong>in</strong>g that <strong>and</strong> are <strong>in</strong>verse proportional functions,<br />

note that the mean Hubble parameter,<br />

is for this Bianchi type mo<strong>de</strong>l FRW mo<strong>de</strong>ls are obta<strong>in</strong>ed if<br />

whereby the flat mo<strong>de</strong>l corresponds to the Bianchi I<br />

curvature term, the open to Bianchi V, <strong>and</strong> closed mo<strong>de</strong>l to Bianchi IX.<br />

Additionally, the cont<strong>in</strong>uity equation yields:<br />

be<strong>in</strong>g a dimensional constant <strong>de</strong>pend<strong>in</strong>g on the fluid present. The<br />

vacuum case is atta<strong>in</strong>ed when<br />

The system of ord<strong>in</strong>ary differential equations, Eqs. (1-12), can be<br />

recast <strong>in</strong> the follow<strong>in</strong>g set:<br />

<strong>and</strong><br />

where <strong>and</strong> we have written the Hubble rates as follows<br />

(similar to the Bianchi type I mo<strong>de</strong>l <strong>de</strong>duced <strong>in</strong> Ref. [14]):

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