Oberdieck–Pixton holomorphic anomaly equation for elliptic fibrations

Let π:XB\pi:X\to B be an elliptic fibration, let kH2(B,Z)\mathsf{k}\in H_2(B,\mathbb{Z}), and let Cg,kπ(γ1,,γn){\mathcal C}^{\pi}_{g,\mathsf{k}}(\gamma_1,\ldots,\gamma_n) be the associated relative Gromov–Witten class. Let ι\iota and jj be the gluing maps for the irreducible and separating boundary strata, respectively, and let Δ!\Delta^! denote pullback along the diagonal of BB. Let ψi\psi_i be the cotangent-line class at the iith marking. Holomorphic anomaly equation conjecture. On Mg,n(B,k){\overline M}_{g,n}(B,\mathsf{k}),

TqCg,kπ(γ1,,γn)=ιΔ!Cg1,kπ(γ1,,γn,1,1)+jΔ!(Cg1,k1π(γS1,1)Cg2,k2π(γS2,1))2i=1nCg,kπ(γ1,,γi1,ππγi,γi+1,,γn)ψi,\begin{aligned} \mathsf{T}_q {\mathcal C}^{\pi}_{g,\mathsf{k}}(\gamma_1,\ldots,\gamma_n)={}&\iota_*\Delta^!{\mathcal C}^{\pi}_{g-1,\mathsf{k}}(\gamma_1,\ldots,\gamma_n,\mathbf{1},\mathbf{1})\\ &+\sum j_*\Delta^!\left({\mathcal C}^{\pi}_{g_1,\mathsf{k}_1}(\gamma_{S_1},\mathbf{1})\boxtimes{\mathcal C}^{\pi}_{g_2,\mathsf{k}_2}(\gamma_{S_2},\mathbf{1})\right)\\ &-2\sum_{i=1}^n{\mathcal C}^{\pi}_{g,\mathsf{k}}(\gamma_1,\ldots,\gamma_{i-1},\pi^*\pi_*\gamma_i,\gamma_{i+1},\ldots,\gamma_n)\cdot\psi_i, \end{aligned}

with the separating sum over g=g1+g2g=g_1+g_2, {1,,n}=S1S2\{1,\ldots,n\}=S_1\sqcup S_2, and k=k1+k2\mathsf{k}=\mathsf{k}_1+\mathsf{k}_2. This equation describes the failure of holomorphicity through boundary gluing and descendant terms; it is part of the general conjectural structure, with special geometries established in the paper.

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Primary source

Georg Oberdieck and Aaron Pixton, “Gromov-Witten theory of elliptic fibrations: Jacobi forms and holomorphic anomaly equations”, arXiv:1709.01481 (2018).

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