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

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

which <strong>in</strong> the present case has the solution<br />

i.e., the equilibrium distribution is <strong>in</strong><strong>de</strong>ed ma<strong>in</strong>ta<strong>in</strong>ed which proves the<br />

consistency of our approach. The particle energy changes from E =<br />

const for to The set of equations (22)–(25)<br />

represents an exactly solvable mo<strong>de</strong>l of a <strong>de</strong>flationary transition from<br />

an <strong>in</strong>itial <strong>de</strong> Sitter phase to a subsequent radiation dom<strong>in</strong>ated FLRW<br />

period, both macroscopically <strong>and</strong> microscopically. This transition is<br />

accompanied by a characteristic change of the “symmetry” condition<br />

(14) with (15) from<br />

characteriz<strong>in</strong>g a “projector-conformal timelike Kill<strong>in</strong>g vector” [7], to<br />

In or<strong>de</strong>r to clarify <strong>in</strong> which sense the modification (9) of the conformal<br />

symmetry is a symmetry aga<strong>in</strong>, we <strong>in</strong>troduce the “optical metric” (cf.<br />

[11, 12, 13])<br />

where plays the role of a refraction <strong>in</strong><strong>de</strong>x of the medium which <strong>in</strong> the<br />

present case changes monotonically from for to<br />

for For we have Optical metrics are known<br />

to be helpful <strong>in</strong> simplify<strong>in</strong>g the equations of light propagation <strong>in</strong> isotropic<br />

refractive media. With respect to optical metrics light propagates as <strong>in</strong><br />

vacuum. Here we <strong>de</strong>monstrate that such type of metrics, <strong>in</strong> particular<br />

their symmetry properties, are also useful <strong>in</strong> relativistic gas dynamics.<br />

Namely, it is easy to realize that the first relation (23) is equivalent to<br />

The quantity is a CKV of the optical metric This clarifies <strong>in</strong><br />

which sense the modification of the conformal symmetry is aga<strong>in</strong> a symmetry.<br />

The transition from a <strong>de</strong> Sitter phase to a FLRW period may<br />

be regar<strong>de</strong>d as a specific non–equilibrium configuration which microscopically<br />

is characterized by an equilibrium distribution function <strong>and</strong>

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