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Riemannian geometry on the quantomorphism group

Published 20 Feb 2013 in math.DG | (1302.5075v1)

Abstract: We are interested in the geometry of the group $\mathcal{D}q(M)$ of diffeomorphisms preserving a contact form $\theta$ on a manifold $M$. We define a Riemannian metric on $\mathcal{D}_q(M)$, compute the corresponding geodesic equation, and show that solutions exist for all time and depend smoothly on initial conditions. In certain special cases (such as on the 3-sphere), the geodesic equation is a simplified version of the quasigeostrophic equation, so we obtain a new geodesic interpretation of this geophysical system. We also show that the genuine quasigeostrophic equation on $S2$ can be obtained as an Euler-Arnold equation on a one-dimensional central extension of $T{\id}\mathcal{D}q(M)$, and that our global existence result extends to this case. If $E$ is the Reeb field of $\theta$ and $\mu$ is the volume form, assumed compatible in the sense that $\text{div} E=0$, we show that $\mathcal{D}_q(M)$ is a smooth submanifold of $\mathcal{D}{E,\mu}(M)$, the space of diffeomorphisms preserving the vector field $E$ and the volume form $\mu$, in the sense of $Hs$ Sobolev completions. The latter manifold is related to symmetric motion of ideal fluids. We further prove that the corresponding geodesic equations and projections are $C{\infty}$ objects in the Sobolev topology.

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