Torsion-dependent Bott–Chern-type decomposition for arbitrary Spin(7)-structures
Construct an operator \(D^{\Phi}_T:C^{\infty}(M)\to\Omega^4_1(M)\oplus\Omega^4_{35}(M)\), together with a suitable first-order differential operator \(d_T\) and harmonic-section space \(H^{\Phi}_T\), such that for an arbitrary Spin(7)-structure with torsion one has \((\Omega^4_1(M)\oplus\Omega^4_{35}(M))\cap\ker d_T=\operatorname{Im}(D^{\Phi}_T)\oplus H^{\Phi}_T\).
References
Find an operator D{\Phi}_T: C{\infty}(M)\rightarrow \Omega4_1(M)\oplus \Omega4_{35}(M) such that (\Omega4_1(M)\oplus \Omega4_{35}(M)) \cap \ker d_T = \Ima(D{\Phi}_T)\oplus H{\Phi}_T, for some suitable first-order differential operator d_T and "harmonic sections" H{\Phi}_T.
— A $dd^Φ$-Lemma and Bott--Chern-type Cohomology for Spin(7)-Manifolds
(2609.04156 - Dwivedi et al., 3 Sep 2026) in Section 7, subsection “Future questions,” first displayed Question