Abstract
We analyze the magnetic field of electroweak dumbbells. While the magnetic field of the untwisted dumbbell is given by the usual dipole formula and falls off as $1/{r}^{3}$, dumbbells with twist have a novel twisted magnetic field that only falls off as $\mathrm{cos}\ensuremath{\theta}/{r}^{2}$ (in spherical coordinates). We comment on the relevance of twisted electroweak dumbbells for understanding the coherence of the magnetic field generated at the electroweak phase transition.
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