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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 243<br />

3.3. THE SPECTRAL INDICES<br />

In general, if the approximation neglect<strong>in</strong>g the right h<strong>and</strong> si<strong>de</strong>s of<br />

Eqs. (2) is taken <strong>in</strong>to account, expressions for the spectral <strong>in</strong>dices at any<br />

or<strong>de</strong>r are easy to be <strong>de</strong>rived not<strong>in</strong>g that <strong>in</strong> these cases expression (25)<br />

always vanishes:<br />

where, are or <strong>and</strong> is correspond<strong>in</strong>gly given by Eqs. (26)<br />

<strong>and</strong> (31). This way it is obta<strong>in</strong>ed<br />

An alternative for more general mo<strong>de</strong>ls. In case it comes out<br />

that Eqs. (35), (36) <strong>and</strong> (37) are also a good approximation for more<br />

general <strong>in</strong>flationary potentials, then <strong>in</strong> the fashion it was done <strong>in</strong> Sec. 2.2,<br />

more general expressions for the spectral <strong>in</strong>dices can be <strong>de</strong>rived.<br />

Un<strong>de</strong>r generalized power–law approximation, for the scalar <strong>in</strong><strong>de</strong>x we<br />

have<br />

<strong>and</strong> to third or<strong>de</strong>r, expression (24) reduces to<br />

Correspond<strong>in</strong>gly, for the tensorial <strong>in</strong><strong>de</strong>x,<br />

<strong>and</strong> its obta<strong>in</strong>ed,<br />

For the scalar amplitu<strong>de</strong>s of the generalized slow–roll approximation,

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