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

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<strong>Scalar</strong> field dark matter 179<br />

where is the Ricci tensor, the <strong>de</strong>term<strong>in</strong>ant of the metric,<br />

<strong>and</strong> a semicolon st<strong>and</strong>s for covariant <strong>de</strong>rivative accord<strong>in</strong>g to the<br />

background space-time;<br />

Assum<strong>in</strong>g the fiat curve condition <strong>in</strong> the scalar dark matter hypothesis,<br />

we are <strong>in</strong> the position to write down the set of field equations. Us<strong>in</strong>g<br />

the metric, the Kle<strong>in</strong> Gordon equation reads<br />

<strong>and</strong> the E<strong>in</strong>ste<strong>in</strong> equations are<br />

In or<strong>de</strong>r to solve equations (30–32), observe that the comb<strong>in</strong>ation of the<br />

previous equations<br />

implies<br />

This is a very important result, namely the scalar potential goes always<br />

as for a spherically symmetric metric with the flat curve condition.<br />

It is remarkable that this behavior of the stress tensor co<strong>in</strong>ci<strong>de</strong>s with the<br />

expected behavior of the energy <strong>de</strong>nsity of the dark matter <strong>in</strong> a galaxy.<br />

We can go further <strong>and</strong> solve the field equations, the general solution of<br />

equations (30-32) is<br />

be<strong>in</strong>g an <strong>in</strong>tegration constant <strong>and</strong> we can thus <strong>in</strong>tegrate the function<br />

Nevertheless, <strong>in</strong> this letter we consi<strong>de</strong>r the most simple solution of<br />

the field equations with Observe that for this particular solution<br />

the stress tensor goes like The energy momentum tensor is ma<strong>de</strong><br />

essentially of two parts. One is the scalar potential <strong>and</strong> the other one<br />

conta<strong>in</strong>s products of the <strong>de</strong>rivatives of the scalar field, both go<strong>in</strong>g as<br />

. Furthermore, as this means that imply<strong>in</strong>g<br />

that the scalar potential is exponential such as has been

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