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

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

equations are equivalent to the Ernst equation<br />

for the complex Ernst potential where the<br />

imag<strong>in</strong>ary part is related to the metric coefficient a via<br />

<strong>and</strong><br />

The boundary value problem for the Ernst potential is <strong>de</strong>scribed <strong>in</strong> <strong>de</strong>tail<br />

<strong>in</strong>[7]. These theta functions were first <strong>in</strong>troduced by Rosenha<strong>in</strong>[8] <strong>and</strong><br />

are a generalization of the Jacobian theta functions. They <strong>de</strong>pend on five<br />

arguments: two ma<strong>in</strong> arguments <strong>and</strong> three moduli. The <strong>de</strong>f<strong>in</strong>ition of the<br />

four Jacobi theta functions <strong>and</strong> of the 16 Rosenha<strong>in</strong> functions<br />

can be found <strong>in</strong> the appendix. The solution <strong>in</strong><br />

terms of ultraelliptic theta functions, is:<br />

The solution exists <strong>and</strong> is regular everywhere outsi<strong>de</strong> the disk <strong>in</strong> the<br />

range where constant<br />

angular velocity, : radius of the<br />

disk). The arguments of the<br />

“theta formula” for <strong>de</strong>pend via ultraelliptic l<strong>in</strong>e <strong>in</strong>tegrals on the normalized<br />

space-time coord<strong>in</strong>ates <strong>and</strong> on the parameter<br />

µ. The functions <strong>and</strong> (also <strong>de</strong>pend<strong>in</strong>g on are explicitly<br />

known. In the follow<strong>in</strong>g the arguments (us<strong>in</strong>g normalized coord<strong>in</strong>ates<br />

are expla<strong>in</strong>ed. The convention for the root is<br />

The functions <strong>and</strong> are<br />

given by<br />

The normalization parameters the moduli of<br />

the theta functions <strong>and</strong> the quantities are <strong>de</strong>f<strong>in</strong>ed via <strong>in</strong>tegrals<br />

on the two sheets of the hyperelliptic Riemann surface (see Figure 1)<br />

related to

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