Consider the space $$W^{2,2}(\Omega ;N)$$ of second order Sobolev mappings $$\ v\ $$ from a smooth domain $$\Omega \subset \mathbb {R}^m$$ to a compact Riemannian manifold N whose Hessian energy $$\int _\Omega |\nabla ^2 v|^2\, dx$$ is finite. Here we are interested in relations between the topology of N and the $$W^{2,2}$$ strong or weak approximability of a $$W^{2,2}$$ map by a sequence of smooth maps from $$\Omega $$ to N. We treat in detail $$W^{2,2}(\mathbb {B}^5,\mathbb {S}^3)$$ where we establish the sequential weak $$W^{2,2}$$ density of $$W^{2,2}(\mathbb {B}^5,\mathbb {S}^3)\,\cap \,{\mathcal C}^\infty $$ . The strong $$W^{2,2}$$ approximability of higher order Sobolev maps has been studied in the recent paper of Bousquet et al. (J. Eur. Math. Soc. (JEMS) 17(4), 763–817, 2015). For an individual map $$v\in W^{2,2}(\mathbb {B}^5,\mathbb {S}^3)$$ , we define a number L(v) which is approximately the total length required to connect the isolated singularities of a strong approximation u of v either to each other or to $$\partial Bx^5$$ . Then $$L(v)=0$$ if and only if v admits $$W^{2,2}$$ strongly approximable by smooth maps. Our critical result, obtained by constructing specific curves connecting the singularities of u, is the bound $$\ L(u)\le c+c\int _{\mathbb {B}^5}|\nabla ^2 u|^2\, dx\ $$ . This allows us to construct, for the given Sobolev map $$v\in W^{2,2}(\mathbb {B}^5,\mathbb {S}^3)$$ , the desired $$W^{2,2}$$ weakly approximating sequence of smooth maps. To find suitable connecting curves for u, one uses the twisting of a u pull-back normal framing on a suitable level surface of u.
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