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

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<strong>Scalar</strong> field dark matter 167<br />

tional curves profile; a motion which does not correspond to the one due<br />

to the observed matter distribution, hence there must be present some<br />

type of dark matter caus<strong>in</strong>g the observed motion. The flat profile of the<br />

rotational curves is maybe the ma<strong>in</strong> feature observed <strong>in</strong> many galaxies.<br />

It is believed that the dark matter <strong>in</strong> galaxies has an almost spherical<br />

distribution which <strong>de</strong>cays like With this distribution of some k<strong>in</strong>d<br />

of matter it is possible to fit the rotational curves of galaxies quite well<br />

[4]. Nevertheless, the ma<strong>in</strong> question of the dark matter problem rema<strong>in</strong>s;<br />

which is the nature of the dark matter <strong>in</strong> galaxies? The problem is not<br />

easy to solve, it is not sufficient to f<strong>in</strong>d out an exotic particle which could<br />

exist <strong>in</strong> galaxies <strong>in</strong> the low energy regime of some theory. It is necessary<br />

to show as well, that this particle (baryonic or exotic) distributes <strong>in</strong> a<br />

very similar manner <strong>in</strong> all these galaxies, <strong>and</strong> f<strong>in</strong>ally, to give some reason<br />

for its existence <strong>in</strong> galaxies.<br />

Recent observations of the lum<strong>in</strong>osity–redshift relation of Ia Supernovae<br />

suggest that distant galaxies are mov<strong>in</strong>g slower than predicted<br />

by Hubble’s law, imply<strong>in</strong>g an accelerated expansion of the Universe [5].<br />

These observations open the possibility to the existence of an energy<br />

component <strong>in</strong> the Universe with a negative equation of state, be<strong>in</strong>g<br />

called dark energy. This result is very important because it<br />

separates the components of the Universe <strong>in</strong>to gravitational (also called<br />

the “matter component” of the Universe) <strong>and</strong> antigravitational (repulsive,<br />

the dark energy). The dark energy would be the currently dom<strong>in</strong>ant<br />

component <strong>in</strong> the Universe <strong>and</strong> its ratio relative to the whole energy<br />

would be The most simple mo<strong>de</strong>l for this dark energy is<br />

cosmological constant <strong>in</strong> which<br />

Observations <strong>in</strong> galaxy clusters <strong>and</strong> dynamical measurements of the<br />

mass <strong>in</strong> galaxies <strong>in</strong>dicate that the matter component of the Universe<br />

is But this component of the Universe <strong>de</strong>composes itself <strong>in</strong><br />

baryons, neutr<strong>in</strong>os, etc. <strong>and</strong> cold dark matter which is responsible of the<br />

formation of structure <strong>in</strong> the Universe. Observations <strong>in</strong>dicate that stars<br />

<strong>and</strong> dust (baryons) represent someth<strong>in</strong>g like 0.3% of the whole matter<br />

of the Universe. The new measurements of the neutr<strong>in</strong>o mass <strong>in</strong>dicate<br />

that neutr<strong>in</strong>os contribute as much with a same quantity as dust. In other<br />

words, say where<br />

represents the dark matter part of the matter contributions which<br />

has a value of The value of the amount of baryonic matter<br />

is <strong>in</strong> concordance with the limits imposed by nucleosynthesis (see<br />

for example [1]). Everyth<strong>in</strong>g seems to agree. Then, this mo<strong>de</strong>l consi<strong>de</strong>rs<br />

a flat Universe full with 95% of unknown matter but<br />

which is of great importance at cosmological level. Moreover, it seems

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