Abstract
Let \(\mathcal {D}_{\omega }^{s}(M)\) denote the group of symplectic diffeomorphisms of a closed symplectic manifold \(M\), which are of Sobolev class \(H^{s}\) for sufficiently high \(s\). When equipped with the \(L^{2}\) metric on vector fields, \(\mathcal {D}_{\omega }^{s}\) becomes an infinite-dimensional Hilbert manifold whose tangent space at a point \(\eta \) consists of \(H^{s}\) sections \(X\) of the pull-back bundle \(\eta ^{*}TM\) for which the corresponding vector field \(u=X\circ \eta ^{-1}\) on \(M\) satisfies \(\mathcal {L}_{u}\omega =0\). Geodesics of the \(L^{2}\) metric are globally defined, so that the \(L^{2}\) metric admits an exponential mapping defined on the whole tangent space. It was shown that this exponential mapping is a non-linear Fredholm map of index zero. Singularities of the exponential map are known as conjugate points and in this paper we construct explicit examples of them on \(\mathcal {D}_{\omega }^{s}(\mathbb {C}P^{n})\). We then solve the Jacobi equation explicitly along a geodesic in \(\mathcal {D}_{\omega }^{s}\), generated by a Killing vector field, and characterize all conjugate points along such a geodesic.
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Notes
A \(\dot{}\) denotes a derivative with respect to \(t\).
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Benn, J. Conjugate points on the symplectomorphism group. Ann Glob Anal Geom 48, 133–147 (2015). https://doi.org/10.1007/s10455-015-9461-5
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DOI: https://doi.org/10.1007/s10455-015-9461-5
Keywords
- Diffeomorphism group
- Hydrodynamics
- Plasma dynamics
- Geodesic
- Conjugate point
- Monoconjugate
- Epiconjugate
- Fredholm map
- Euler equations
- Hilbert manifold