Unboundedness above and below of the Donaldson-Hitchin functionals on $\mathrm{G}_2$- and $\widetilde{\mathrm{G}}_2$-forms
Laurence H. Mayther
TL;DR
This work studies the unboundedness properties of Donaldson–Hitchin functionals associated with $G_2$ and $\widetilde{G}_2$-structures on compact oriented $7$-manifolds (or orbifolds) with boundary. By combining explicit local computations with covering arguments, it shows that $\mathcal{H}_4^{\partial}$, $\widetilde{\mathcal{H}}_3^{\partial}$, and $\widetilde{\mathcal{H}}_4^{\partial}$ are unbounded above and below in a logarithmic sense on $[\psi]_{+}^{\partial}$ (for closed $G_2$ $4$-forms $\psi$), while $\mathcal{H}_3^{\partial}$ is unbounded below on $[\phi]_{+}^{\partial}$. The critical points of these functionals are saddles, and the Laplacian coflow from generic boundary-adhering initial data does not generically converge to torsion-free structures, with the non-convergent set dense in $C^0$. These results remain valid in the orbifold setting, and they yield a partial analogue for $\mathcal{H}_3^{\partial}$ regarding the saddle/flatness structure and convergence behavior. The paper also clarifies the relation between unboundedness and the long-time behavior of the Laplacian coflow, and highlights open questions for the unboundedness of $\mathcal{H}_3^{\partial}$ in full generality.
Abstract
This paper combines explicit local calculations with covering arguments to prove the unboundedness above and below (in a logarithmic sense) of the Donaldson-Hitchin functionals on $\mathrm{G}_2$ 4-forms, $\widetilde{\mathrm{G}}_2$ 3-forms and $\widetilde{\mathrm{G}}_2$ 4-forms, over compact manifolds (or, more generally, orbifolds) with boundary. In addition, the Donaldson-Hitchin functional on $\mathrm{G}_2$ 3-forms over compact manifolds (or orbifolds) with boundary is shown to be unbounded below. As scholia, the critical points of the functionals on $\mathrm{G}_2$ 4-forms, $\widetilde{\mathrm{G}}_2$ 3-forms and $\widetilde{\mathrm{G}}_2$ 4-forms are shown to be saddles, and initial conditions of the Laplacian coflow which do not lead to convergent solutions are shown to be dense.
