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

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

then the function if it exits, can be constructed as a Taylor series<br />

<strong>in</strong> with<strong>in</strong> a f<strong>in</strong>ite neighborhood of X, thus any Kill<strong>in</strong>g vector<br />

of the metric can be expressed as<br />

where <strong>and</strong> the same for all Kill<strong>in</strong>g vectors at the<br />

neighborhood of X, are functions of the metric <strong>and</strong> X. Nevertheless,<br />

whether (4) is solvable for a given set of <strong>in</strong>itial data <strong>and</strong><br />

<strong>de</strong>pends on the above <strong>in</strong>tegrability conditions (10), impos<strong>in</strong>g<br />

l<strong>in</strong>ear relations among <strong>and</strong> at any given po<strong>in</strong>t X. The maximal<br />

dimension of the space of <strong>in</strong>itial data constructed on<br />

be<strong>in</strong>g is reduced by the number of relations<br />

(10). Thus, if there were no relations (10) on the data <strong>and</strong><br />

then each Kill<strong>in</strong>g vector of a given was uniquely<br />

<strong>de</strong>term<strong>in</strong>ed by the <strong>in</strong><strong>de</strong>pen<strong>de</strong>nt quantities <strong>and</strong> <strong>in</strong> number<br />

equal respectively to <strong>and</strong> Hence, a allows for at most<br />

an parameter group of Kill<strong>in</strong>g vectors<br />

The so-called maximally symmetric space or space of constant<br />

curvature, admits the maximal number of Kill<strong>in</strong>g vectors.<br />

Hence, the equations (10) do not impose conditions on <strong>and</strong><br />

at any po<strong>in</strong>t X, <strong>and</strong> therefore they acquire respectively <strong>and</strong><br />

arbitrary values at X. The vanish<strong>in</strong>g of the factor multiply<strong>in</strong>g<br />

<strong>in</strong> (10) yields to the constancy of the scalar curvature R.<br />

3. MAXIMALLY SYMMETRIC SPACES<br />

A maximally symmetric space is, by <strong>de</strong>f<strong>in</strong>ition, a space which admits<br />

a cont<strong>in</strong>uous group of motions of parameters. On the other<br />

h<strong>and</strong>, a maximally symmetric space is characterized, accord<strong>in</strong>g to We<strong>in</strong>berg,<br />

by the follow<strong>in</strong>g property:W379, a maximally symmetric space<br />

is necessarily homogeneous <strong>and</strong> isotropic about all po<strong>in</strong>ts. We<strong>in</strong>berg<br />

worked out <strong>in</strong> <strong>de</strong>tails the structure of the Kill<strong>in</strong>g vectors, which arises<br />

from the the homogeneous <strong>and</strong> isotropic properties of a consi<strong>de</strong>red space:<br />

W378:A metric space is said to be homogeneous if there exit <strong>in</strong>f<strong>in</strong>itesimal<br />

isometries (2) that carry any po<strong>in</strong>t <strong>in</strong>to any other po<strong>in</strong>t<br />

<strong>in</strong> its immediate neighborhood. That is, the metric must admit<br />

Kill<strong>in</strong>g vectors that at any po<strong>in</strong>t take all possible values. In particular,<br />

<strong>in</strong> a one can choose a set of Kill<strong>in</strong>g vectors<br />

with<br />

W378: A metric space is said to be isotropic about a given po<strong>in</strong>t if<br />

there exit <strong>in</strong>f<strong>in</strong>itesimal isometries (2) that leave the po<strong>in</strong>t X fixed,

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