Stable quotient holomorphic anomaly equations for local \u03b2c0^2

Let KP2K\mathbb{P}^2 be the local projective plane, let T=I1KP2(q)T=I^{K\mathbb{P}^2}_1(q) be the mirror coordinate, and let FgSQ\mathcal{F}^{\mathsf{SQ}}_g denote its genus-gg stable quotient invariants. Let A2A_2, C1C_1, and the derivatives with respect to TT be as defined in the source. Holomorphic anomaly equation for local P2\mathbb{P}^2. For g2g\geq2,

1C12FgSQA2=12i=1g1FgiSQTFiSQT+122Fg1SQT2.\frac{1}{C_1^2}\frac{\partial\mathcal{F}^{\mathsf{SQ}}_g}{\partial A_2}=\frac{1}{2}\sum_{i=1}^{g-1}\frac{\partial\mathcal{F}^{\mathsf{SQ}}_{g-i}}{\partial T}\frac{\partial\mathcal{F}^{\mathsf{SQ}}_i}{\partial T}+\frac{1}{2}\frac{\partial^2\mathcal{F}^{\mathsf{SQ}}_{g-1}}{\partial T^2}.

These equations describe the genus recursion predicted by the holomorphic anomaly formalism for stable quotient invariants; no resolution is supplied in the given text.

Sources & referencesView supporting material

Primary source

Hyenho Lho, “Equivariant holomorphic anomaly equation”, arXiv:1807.05503 (2018).

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