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

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 239<br />

2.2. THE SPECTRAL INDICES<br />

To <strong>de</strong>rive the expressions for the spectral <strong>in</strong>dices we <strong>in</strong>troduce here<br />

a variation of the st<strong>and</strong>ard procedure that has the advantage of be<strong>in</strong>g<br />

more comprehensive while <strong>de</strong>al<strong>in</strong>g with the or<strong>de</strong>r of expressions to be<br />

<strong>de</strong>rived us<strong>in</strong>g the slow–roll expansion.<br />

First, let us assume the follow<strong>in</strong>g ansatz for the power spectrum of<br />

general <strong>in</strong>flationary mo<strong>de</strong>ls,<br />

where may be written as a Taylor expansion while is<br />

a general function which, <strong>in</strong> pr<strong>in</strong>ciple, can be non–cont<strong>in</strong>uous <strong>in</strong><br />

Note that any function can be <strong>de</strong>composed <strong>in</strong>to this form. We<br />

must also consi<strong>de</strong>r the follow<strong>in</strong>g function of the slow–roll parameters:<br />

In this expression all of the parameters are to be evaluated at values of<br />

correspond<strong>in</strong>g to The functions <strong>and</strong> can be exp<strong>and</strong>ed <strong>in</strong><br />

Taylor series,<br />

We proceed with the <strong>de</strong>rivation of the equations for the scalar spectral<br />

<strong>in</strong><strong>de</strong>x<br />

From Eq. (15) we obta<strong>in</strong><br />

where<br />

<strong>and</strong> After differentiation,

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