FDCF3D0F683E
Use the Su–Wood Ansatz with $a=1$ and an admissible compact group $G\subset SU(m-1)$ acting on $\mathbb C^{m-1}$ with isotropic orbits of dimension $m-2$. If $\gamma ,\xi $ are the regular (with the smooth extension at a line profile's origin understood) profile curves satisfying equation (1) of the source, its profile map is
The full Lagrangian is the $G$-orbit of the specified linear inclusion of $\check F$ into $\mathbb C^ m$ and translates in $\operatorname {Re}z_ m$. The source uses opposite profile soliton constants for the two factors. It is the induced orbit geometry, not ordinary planar curve shortening, that gives the Anciaux profile equation.
Example 3 uses a shrinker and an expander profile and gives immersed $SO(m-1)$- or $T^{m-2}$-invariant translators. They are unbounded in $\operatorname {Im}z_ m$ and are not almost calibrated. Full embeddedness and properness are not asserted uniformly here. Non-spherical orbit choices must retain the smoothness restrictions of Section 5.4.
The associated motion is translation for every real time. The plotted object is the two-dimensional profile projection used in Figures 1–2, not the full $m$-dimensional Lagrangian. The source explicitly does not claim new complete smooth embedded almost-calibrated translators from this Ansatz.
Sources: [SuWood2026].
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