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Published: August 6, 2022 (6 days ago)

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All of the above examples have been rational. What happens if we want to consider the manifold with boundary $K$. Again we expect the hyperbolic structure to look like that of a conic bundle over $K$ with the hyperbolic structure over the cone points. We take some such example and do an ${mathbb{R}}$-split along the common boundary component. This gives a hyperbolic structure on the resulting Riemann surface with an ${mathbb{R}}$ action that is either parabolic or hyperbolic or nontransitive. This is exactly the situation that we would like to understand for $3$-manifolds with non-empty boundary. However, if we were to take the truncation of the hyperbolic metric for any of these examples and restrict it to the boundary component to obtain a hyperbolic metric on the compact manifold with boundary, the metric on the boundary will be complete. For the Löbell cone (Figure [lobell]) this seems to be a fairly natural result. In this case the hyperbolic structure on $S^2 times {mathbb{R}}$ extends to a cone over $S^2 times S^1$ with boundary $S^2 times S^1$ by taking the product of the hyperb

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