A string theory question on my general relativity problem set:
Metric is given as ds2=−A(r)dt2+B(r)dr2+r2dθ2.
a) Solve the vacuum equations and find the metric around the massive source assuming that the Ricci curvature vanishes. Use a change of coordinates to put the metric in the form,
ds2=−dt2+dr2+C(r)r2dθ2
b) Consider the metric on a spatial slice (t = constant). Use the relationship between curvature and parallel transport to determine the total curvature that must be contained in the region containing the source if parallel transport around a single cosmic string rotates a vector by 2π/N.
c) Write the metric at a large distance from a configuration of k sources, assuming each separately gives rise to the metric described in the previous part. What is the maximum number of parallel such cosmic strings that can inhabit space-time? With this maximum number of cosmic strings, what is the total curvature over a 2D surface perpendicular to the strings?
--I attempted the first part, found all connections and Ricci tensor components. Requiring that the Ricci tensor be zero. I attempted to get what seemed to be a mess of algebra to solve for B(r) and A(r). But I didn't really get it to work. Regardless, I know that in the form C(r) is given by a few books to be something of the form 1−4μ, whose interpretation as canonical spacetime makes enough sense to me. The latter two parts are where I'm really at a loss.
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