Symmetries in LDDMM with higher order momentum distributions
This work addresses theoretical advancements in mathematical image registration for researchers in computational anatomy and geometric mechanics, but it appears incremental as it builds on existing LDDMM frameworks.
The paper tackles the problem of extending the Large Deformation Diffeomorphic Metric Mapping (LDDMM) formulation for image registration by considering particles that do more than just translate image data, focusing on symmetries in higher-order momentum distributions. It results in the construction of a tower of Lie groups corresponding to preserving k-th order jet-data, leading to finite-dimensional reduced configuration spaces and conserved momenta via Noether's theorem.
In some implementations of the Large Deformation Diffeomorphic Metric Mapping formulation for image registration we consider the motion of particles which locally translate image data. We then lift the motion of the particles to obtain a motion on the entire image. However, it is certainly possible to consider particles which do more than translate, and this is what will be described in this paper. As the unreduced Lagrangian associated to EPDiff possesses $\Diff(M)$ symmetry, it must also exhibit $G \subset \Diff(M)$ symmetry, for any Lie subgroup. In this paper we will describe a tower of Lie groups $G^{(0)} \subseteq G^{(1)} \subseteq G^{(2)} \subseteq...$ which correspond to preserving $k$-th order jet-data. The reduced configuration spaces $Q^{(k)} := \Diff(M) / G^{(k)}$ will be finite-dimensional (in particular, $Q^{(0)}$ is the configuration manifold for $N$ particles in $M$). We will observe that $G^{(k)}$ is a normal subgroup of $G^{(0)}$ and so the quotient $G^{(0)} / G^{(k)}$ is itself a (finite dimensional) Lie group which acts on $Q^{(k)}$. This makes $Q^{(k)}$ a principle bundle over $Q^{(0)}$ and the reduced geodesic equations on $Q^{(k)}$ will possess $G^{(0)} / G^{(k)}$-symmetry. Noether's theorem implies the existence of conserved momenta for the reduced system on $T^{\ast}Q^{(k)}$.