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

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

i.e., particle number <strong>de</strong>nsity <strong>and</strong> temperature are the <strong>in</strong><strong>de</strong>pen<strong>de</strong>nt thermodynamical<br />

variables. Differentiat<strong>in</strong>g the latter relation, us<strong>in</strong>g the<br />

balances (4) <strong>and</strong> restrict<strong>in</strong>g ourselves to a constant entropy per particle,<br />

we obta<strong>in</strong> the cool<strong>in</strong>g rate<br />

Compar<strong>in</strong>g the expressions <strong>in</strong> (2) <strong>and</strong> (6) for the temperature evolution<br />

we f<strong>in</strong>d that they are consistent for<br />

In the special case we recover that<br />

is a conformal Kill<strong>in</strong>g vector (CKV) of the metric<br />

Equation (7) represents a modification of the CKV condition <strong>in</strong> (8) even<br />

<strong>in</strong> the homogeneous <strong>and</strong> isotropic case where <strong>and</strong><br />

S<strong>in</strong>ce the CKV property of is known to be related to the dynamics<br />

of a st<strong>and</strong>ard radiation dom<strong>in</strong>ated universe, the question arises to what<br />

extent the replacement<br />

<strong>in</strong> (7) gives rise to a modified cosmological dynamics. In particular, it is<br />

of <strong>in</strong>terest to explore whether this modification possibly admits phases<br />

of accelerated expansion of the universe. To clarify this question we first<br />

recall that the CKV property of may be obta<strong>in</strong>ed as a “global” equilibrium<br />

condition <strong>in</strong> relativistic gas dynamics. Then we ask whether the<br />

more general case correspond<strong>in</strong>g to the modification (9) can be <strong>de</strong>rived<br />

<strong>in</strong> a gas dynamical context as well.<br />

3. GAS DYNAMICS<br />

Relativistic gas dynamics is based on Boltzmann’s equation for the<br />

one–particle distribution function

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