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

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Revisit<strong>in</strong>g the calculation of <strong>in</strong>flationary perturbations 245<br />

For the spectral <strong>in</strong>dices one can see that substitution of relations (48) <strong>in</strong><br />

Eqs. (38) <strong>and</strong> (40), as well as <strong>in</strong> Eqs. (42) <strong>and</strong> (44), yield<br />

Another <strong>in</strong>flationary scenario where precise predictions for the spectra<br />

amplitu<strong>de</strong>s <strong>and</strong> <strong>in</strong>dices can be done is natural <strong>in</strong>flation [11]. In this case,<br />

the potential is given by,<br />

where <strong>and</strong> are mass scales. For simplicity we choose the plus sign <strong>in</strong><br />

the rema<strong>in</strong><strong>in</strong>g calculations. The po<strong>in</strong>t here is to analyze <strong>in</strong>flation near<br />

the orig<strong>in</strong> so that the small–angle approximation applies, i.e., In<br />

this case the slow–roll parameters are,<br />

As it can be observed, <strong>in</strong> this approximation natural <strong>in</strong>flation belongs to<br />

the class of mo<strong>de</strong>ls that fulfill the conditions of the generalized slow–roll<br />

approximation. With the values of the parameters given above, Eq. (6)<br />

can be used with the correspond<strong>in</strong>g After exp<strong>and</strong><strong>in</strong>g <strong>and</strong><br />

truncat<strong>in</strong>g at the proper or<strong>de</strong>r<br />

is obta<strong>in</strong>ed, consistent with Eq. (37). With this same set of assumptions,<br />

Eq. (40) <strong>and</strong> (46) are reduced to<br />

the well known result for natural <strong>in</strong>flation.<br />

5. CONCLUSIONS<br />

In this paper we <strong>in</strong>troduced a formalism which allows to <strong>in</strong>crease the<br />

precision for the theoretical predictions of spectra of <strong>in</strong>flationary perturbations<br />

for two specific classes of <strong>in</strong>flationary mo<strong>de</strong>ls. The method

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