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

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238 EXACT SOLUTIONS AND SCALAR FIELDS IN GRAVITY<br />

where is given by<br />

<strong>and</strong> is the wavenumber correspond<strong>in</strong>g to the scale match<strong>in</strong>g the Hubble<br />

radius. Exp<strong>and</strong><strong>in</strong>g solution (6) with given by <strong>and</strong><br />

truncat<strong>in</strong>g the results to first or<strong>de</strong>r <strong>in</strong> <strong>and</strong> the st<strong>and</strong>ard general<br />

expression for the scalar spectrum is obta<strong>in</strong>ed,<br />

where is a numerical constant, <strong>and</strong> is the<br />

Euler constant that arises when exp<strong>and</strong><strong>in</strong>g the Gamma function. Eq. (8)<br />

is called the next–to–lead<strong>in</strong>g or<strong>de</strong>r expression for the spectrum amplitu<strong>de</strong>s<br />

of scalar perturbations, <strong>and</strong> from it the lead<strong>in</strong>g or<strong>de</strong>r is recovered<br />

by neglect<strong>in</strong>g first or<strong>de</strong>r terms for <strong>and</strong><br />

The correspond<strong>in</strong>g equation of motion for the tensorial mo<strong>de</strong>s is<br />

where,<br />

Neglect<strong>in</strong>g any or<strong>de</strong>r of higher than the first one, Eq. (10) can be<br />

written as<br />

where,<br />

This way, Eq. (9) can be also approximated as a Bessel equation with<br />

solution,<br />

Substitut<strong>in</strong>g µ, given by Eq. (12) <strong>in</strong> Eq. (13), exp<strong>and</strong><strong>in</strong>g on <strong>and</strong> truncat<strong>in</strong>g<br />

to first or<strong>de</strong>r, the Stewart–Lyth next–to–lead<strong>in</strong>g or<strong>de</strong>r result is<br />

obta<strong>in</strong>ed<br />

The lead<strong>in</strong>g or<strong>de</strong>r equation is recovered by neglect<strong>in</strong>g

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