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

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

where <strong>and</strong> satisfies<br />

Self–dual (anti–self–dual) Riemann tensors are <strong>de</strong>f<strong>in</strong>ed as well <strong>in</strong> terms<br />

of the self–dual (anti–self–dual) component of the sp<strong>in</strong> connection<br />

as<br />

with<br />

The Lagrangian (4) can be written obviously as where<br />

The Eucli<strong>de</strong>an partition function is <strong>de</strong>f<strong>in</strong>ed as [5]<br />

which satisfies a factorization where<br />

It is an easy matter to see from action (4) that the partition function<br />

(8) is <strong>in</strong>variant un<strong>de</strong>r comb<strong>in</strong>ed shifts of <strong>and</strong> for<br />

<strong>in</strong> the case of sp<strong>in</strong> manifolds <strong>and</strong> for non-sp<strong>in</strong> manifolds<br />

In or<strong>de</strong>r to f<strong>in</strong>d a S–dual theory to (4) we follow references [2]. The<br />

procedures are similar to those presented <strong>in</strong> the Introduction for Yang–<br />

Mills theories. We beg<strong>in</strong> by propos<strong>in</strong>g a parent Lagrangian

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