$G$-Strands

A $G$-strand is a map $g(t,s):\mathbb{R}\times \mathbb{R}\to G$ for a Lie group $G$ that follows from Hamilton’s principle for a certain class of $G$-invariant Lagrangians. The SO(3)-strand is the $G$-strand version of the rigid body equation and it may be regarded physically as a continuous spin chain. Here, $SO(3{)}_K$-strand dynamics for ellipsoidal rotations is derived as an Euler-Poincar'e system for a certain class of variations and recast as a Lie-Poisson system for coadjoint flow with the same Hamiltonian structure as for a perfect complex fluid. For a special Hamiltonian, the $SO(3{)}_K$-strand is mapped into a completely integrable generalization of the classical chiral model for the SO(3)-strand. Analogous results are obtained for the $Sp(2)$-strand. The $Sp(2)$-strand is the $G$-strand version of the $Sp(2)$ Bloch-Iserles ordinary differential equation, whose solutions exhibit dynamical sorting. Numerical solutions show nonlinear interactions of coherent wave-like solutions in both cases. $\mathrm{D}\mathrm{i}\mathrm{f}\mathrm{f}(\mathbb{R})$-strand equations on the diffeomorphism group $G=\mathrm{D}\mathrm{i}\mathrm{f}\mathrm{f}(\mathbb{R})$ are also introduced and shown to admit solutions with singular support (e.g., peakons).