In this paper, we initiate the study of finite energy equivariant wave maps from the (1+3)-dimensional spacetime $\mathbb R \times (\mathbb R \times ^2) \rightarrow ^3\mathbb R \times (\mathbb R \times ^2)$ is given by ds^2 = -dt^2 + dr^2 + (r^2 + 1) \left ( d \theta^2 + \sin^2 \theta d \varphi^2 \right ), \quad t,r \in , (\theta,\varphi) \in ^2. The constant time slices are each given by the Riemannian manifold $\mathcal M := \mathbb R \times ^2$ with metric ds^2 = dr^2 + (r^2 + 1) \left ( d \theta^2 + \sin^2 \theta d \varphi^2 \right ). The Riemannian manifold contains two asymptotically Euclidean ends at that are connected by a spherical throat of area at . The spacetime $\mathbb R \times \mathcal M$ is a simple example of a wormhole geometry in general relativity. In this work we will consider 1–equivariant or corotational wave maps. Each corotational wave map can be indexed by its topological degree . For each , there exists a unique energy minimizing corotational harmonic map of degree . In this work, we show that modulo a free radiation term, every corotational wave map of degree converges strongly to . This resolves a conjecture made by Bizon and Kahl in the corotational case.

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