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A comparison among different constructions in $$\mathbb {H}^2 \cong {\mathbb {R}}^8$$ H 2 ≅ R 8 of the quaternionic 4-form $$\Phi _{\text {Sp}(2)\text {Sp}(1)}$$ Φ Sp ( 2 ) Sp ( 1 ) and of the Cayley calibration $$\Phi _{\text {Spin}(7)}$$ Φ Spin ( 7 ) shows that one can start for them from the same collections of “Kähler 2-forms”, entering both in quaternion Kähler and in $$\text {Spin}(7)$$ Spin ( 7 ) geometry. This comparison relates with the notions of even Clifford structure and of Clifford system. Going to dimension 16, similar constructions allow to write explicit formulas in $$\mathbb {R}^{16}$$ R 16 for the canonical 4-forms $$\Phi _{\text {Spin}(8)}$$ Φ Spin ( 8 ) and $$\Phi _{\text {Spin}(7)\text {U}(1)}$$ Φ Spin ( 7 ) U ( 1 ) , associated with Clifford systems related with the subgroups $$\text {Spin}(8)$$ Spin ( 8 ) and $$\text {Spin}(7)\text {U}(1)$$ Spin ( 7 ) U ( 1 ) of $$\text {SO}(16)$$ SO ( 16 ) . We characterize the calibrated 4-planes of the 4-forms $$\Phi _{\text {Spin}(8)}$$ Φ Spin ( 8 ) and $$\Phi _{\text {Spin}(7)\text {U}(1)}$$ Φ Spin ( 7 ) U ( 1 ) , extending in two different ways the notion of Cayley 4-plane to dimension 16.
A comparison among different constructions in $$\mathbb {H}^2 \cong {\mathbb {R}}^8$$ H 2 ≅ R 8 of the quaternionic 4-form $$\Phi _{\text {Sp}(2)\text {Sp}(1)}$$ Φ Sp ( 2 ) Sp ( 1 ) and of the Cayley calibration $$\Phi _{\text {Spin}(7)}$$ Φ Spin ( 7 ) shows that one can start for them from the same collections of “Kähler 2-forms”, entering both in quaternion Kähler and in $$\text {Spin}(7)$$ Spin ( 7 ) geometry. This comparison relates with the notions of even Clifford structure and of Clifford system. Going to dimension 16, similar constructions allow to write explicit formulas in $$\mathbb {R}^{16}$$ R 16 for the canonical 4-forms $$\Phi _{\text {Spin}(8)}$$ Φ Spin ( 8 ) and $$\Phi _{\text {Spin}(7)\text {U}(1)}$$ Φ Spin ( 7 ) U ( 1 ) , associated with Clifford systems related with the subgroups $$\text {Spin}(8)$$ Spin ( 8 ) and $$\text {Spin}(7)\text {U}(1)$$ Spin ( 7 ) U ( 1 ) of $$\text {SO}(16)$$ SO ( 16 ) . We characterize the calibrated 4-planes of the 4-forms $$\Phi _{\text {Spin}(8)}$$ Φ Spin ( 8 ) and $$\Phi _{\text {Spin}(7)\text {U}(1)}$$ Φ Spin ( 7 ) U ( 1 ) , extending in two different ways the notion of Cayley 4-plane to dimension 16.
Let M be an oriented three-dimensional Riemannian manifold. We define a notion of vorticity of local sections of the bundle SO ( M ) → M {\mathrm{SO}(M)\rightarrow M} of all its positively oriented orthonormal tangent frames. When M is a space form, we relate the concept to a suitable invariant split pseudo-Riemannian metric on Iso o ( M ) ≅ SO ( M ) {\mathrm{Iso}_{o}(M)\cong\mathrm{SO}(M)} : A local section has positive vorticity if and only if it determines a space-like submanifold. In the Euclidean case we find explicit homologically volume maximizing sections using a split special Lagrangian calibration. We introduce the concept of optimal frame vorticity and give an optimal screwed global section for the three-sphere. We prove that it is also homologically volume maximizing (now using a common one-point split calibration). Besides, we show that no optimal section can exist in the Euclidean and hyperbolic cases.
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