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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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Inflation with a blue eigenvalue spectrum 187<br />

po<strong>in</strong>t. Thus some specific eigenvalues of the family of<br />

solutions can be related rather accurately to exist<strong>in</strong>g as well as future<br />

observations.<br />

2. SPATIALLY FLAT INFLATIONARY<br />

UNIVERSE<br />

In the E<strong>in</strong>ste<strong>in</strong> frame, a rather general class of <strong>in</strong>flationary mo<strong>de</strong>ls<br />

can be mo<strong>de</strong>led by the Lagrangian <strong>de</strong>nsity:<br />

where R is the curvature scalar, the scalar field, the self–<strong>in</strong>teraction<br />

potential <strong>and</strong> the gravitational coupl<strong>in</strong>g constant. Natural<br />

units with are used <strong>and</strong> our signature for the metric is<br />

(+1, –1, –1, –1) as it is common <strong>in</strong> particle physics.<br />

For the flat Robertson-Walker metric favored by<br />

recent observations, the evolution of the generic <strong>in</strong>flationary mo<strong>de</strong>l (1)<br />

is <strong>de</strong>term<strong>in</strong>ed by the autonomous first or<strong>de</strong>r equations<br />

where For this system of equation, <strong>de</strong> Sitter<br />

<strong>in</strong>flation with is a s<strong>in</strong>gular, but well–known <strong>and</strong> trivial subcase,<br />

cf. Ref. [17]. Otherwise, for we can simply reparametrize<br />

the <strong>in</strong>flationary potential <strong>in</strong> terms<br />

of the Hubble expansion rate as the new “<strong>in</strong>verse time”<br />

coord<strong>in</strong>ate. For this non-s<strong>in</strong>gular coord<strong>in</strong>ate transformation, the term<br />

reduces to the graceful exit function<br />

<strong>and</strong> the follow<strong>in</strong>g general metric <strong>and</strong> scalar field solution of (2) emerges<br />

[5, 6]:<br />

Once we know from some experimental <strong>in</strong>put, we can (formally)<br />

<strong>in</strong>vert (4) <strong>in</strong> or<strong>de</strong>r to recover from the cha<strong>in</strong> of substitutions<br />

the <strong>in</strong>flaton potential <strong>in</strong> a simple <strong>and</strong> rather elegant manner.

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