Mirror identification of the corrected differential via polyvector fields
Establish that, under mirror symmetry, the corrected differential δ + {μ^0,·} on the family Floer complex corresponds to deforming the Čech complex of polyvector fields C^*(Y^0; Λ^*TY^0) to the polyvector fields (or an appropriate noncommutative analogue) on the corrected mirror space.
References
Conjecturally, under mirror symmetry this amounts to deforming the \v{C}ech complex of polyvector fields $C(Y0;\Lambda^ TY0)$ to arrive at polyvector fields (or their appropriate noncommutative analogue) on the corrected mirror.
                — Lagrangian Floer theory, from geometry to algebra and back again
                
                (2510.22476 - Auroux, 26 Oct 2025) in Section 3.1, “Floer theory for families of Lagrangians,” same subsection on negative Maslov index and extended deformations