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

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Inflation with a blue eigenvalue spectrum 189<br />

polynomial of first <strong>de</strong>gree, where<br />

necessarily satisfies the additional constra<strong>in</strong>t due to the<br />

nonl<strong>in</strong>earity of the Abel equation. Mathematically, this transformation<br />

improves the or<strong>de</strong>r of the polynomial by one <strong>in</strong> comparison with (3.1),<br />

where the solution is just a polynomial of zero <strong>de</strong>gree. This first or<strong>de</strong>r<br />

polynomial corresponds to where is aga<strong>in</strong> given by<br />

(9). S<strong>in</strong>ce is <strong>de</strong>term<strong>in</strong>ed due to the additional constra<strong>in</strong>t mentioned<br />

above, cf. Ref. [21], the spectral <strong>in</strong><strong>de</strong>x is now completely fixed by the<br />

Euler constant as<br />

In or<strong>de</strong>r to circumvent this ‘no-go’ theorem for polynomial solutions, we<br />

shall <strong>in</strong>troduce a different transformation which leads us to new solutions<br />

<strong>in</strong> form of an <strong>in</strong>f<strong>in</strong>ite series.<br />

3.1. SOLUTIONS WITH A BLUE SPECTRUM<br />

If we assume that with Eq. (6) can be rearranged<br />

to<br />

where If we try the ansatz it turns out that<br />

the odd powers have to vanish. This can be traced back to the fact<br />

that (13) is <strong>in</strong>variant un<strong>de</strong>r reflections only for even functions<br />

For even powers, this boils down to the follow<strong>in</strong>g Taylor<br />

expansion:<br />

where is a positive <strong>in</strong>teger, which labels the first non-constant term <strong>in</strong><br />

our expansion <strong>and</strong> thus dist<strong>in</strong>guishes the different subclasses of solutions.<br />

Hence, the series for starts as for<br />

the case as <strong>and</strong> so on. In all cases,<br />

the coefficient of zeroth or<strong>de</strong>r is aga<strong>in</strong> <strong>de</strong>term<strong>in</strong>ed algebraically<br />

by a via Eq. (9); or, as we shall show below, is <strong>de</strong>term<strong>in</strong>ed by the<br />

next higher or<strong>de</strong>r, <strong>and</strong> the zeroth or<strong>de</strong>r establishes<br />

In or<strong>de</strong>r we f<strong>in</strong>d the follow<strong>in</strong>g discrim<strong>in</strong>at<strong>in</strong>g relation<br />

due to the nonl<strong>in</strong>earity of the Abel type equation. This recursion relation<br />

implies or the new additional

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