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

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

The constancy of R results from the Bianchi i<strong>de</strong>ntity<br />

Contract<strong>in</strong>g <strong>in</strong> <strong>and</strong> one obta<strong>in</strong>s<br />

contract<strong>in</strong>g aga<strong>in</strong> <strong>in</strong> <strong>and</strong> one gets<br />

substitut<strong>in</strong>g (17) <strong>in</strong> the above equation, one arrives at<br />

Hence any space of three or more dimensions <strong>in</strong> which (17) holds everywhere<br />

will have R constant. Moreover, for maximally symmetric spaces<br />

of two dimensions the scalar curvature R occurs to be also constant. A<br />

necessary <strong>and</strong> sufficient condition that the curvature at every po<strong>in</strong>t of<br />

space be <strong>in</strong><strong>de</strong>pen<strong>de</strong>nt of the orientation is that the Riemann tensor is<br />

expressible as (18).<br />

Introduc<strong>in</strong>g the curvature constant K, one has<br />

On the other h<strong>and</strong>, via the homogeneous property at a given po<strong>in</strong>t<br />

<strong>in</strong> a maximally symmetric space, there exist <strong>in</strong><strong>de</strong>pen<strong>de</strong>nt Kill<strong>in</strong>g vectors<br />

for which takes any values one likes, thus<br />

which by cyclic permutation of <strong>and</strong> gives<br />

which, by virtue of the properties of the Riemann tensor, is i<strong>de</strong>ntically<br />

zero, <strong>and</strong> therefore it gives no <strong>in</strong>formation.<br />

It becomes then clear that maximally symmetric spaces are unique <strong>in</strong><br />

the sense that any two maximally symmetric spaces of the same signature<br />

<strong>and</strong> the same constant curvature are isometric <strong>and</strong> have the same<br />

<strong>in</strong>tr<strong>in</strong>sic properties, <strong>and</strong> that the equations of the isometric correspon<strong>de</strong>nce<br />

<strong>in</strong>volve arbitrary constants.

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