Hodge–FVH correspondence for special cubic Hodge integrals

Let H(t;p,q,r;ϵ)\mathcal{H}({\bf t};p,q,r;\epsilon) be the cubic Hodge free energy, let w=ϵ2t02H(t;p,q,r;ϵ)w=\epsilon^2\partial_{t_0}^2\mathcal{H}({\bf t};p,q,r;\epsilon), and let Zcubic(t;p,q,r;ϵ)=exp(H(t;p,q,r;ϵ))Z_{\rm cubic}({\bf t};p,q,r;\epsilon)=\exp(\mathcal{H}({\bf t};p,q,r;\epsilon)) be the corresponding cubic Hodge partition function. The cubic Hodge hierarchy is the integrable hierarchy satisfied by ww, deforming the Riemann hierarchy; the fractional Volterra hierarchy (FVH) is the hierarchy appearing in the conjectured correspondence. Hodge–FVH correspondence. The Hodge hierarchy for the special cubic Hodge integrals is equivalent, under a certain Miura-type transformation, to the fractional Volterra hierarchy (FVH). Furthermore, the corresponding cubic Hodge partition function gives a tau function of the FVH. This conjecture proposes an integrable-systems description of special cubic Hodge integrals, identifying their Hodge hierarchy with the fractional Volterra hierarchy and interpreting the cubic Hodge partition function as a tau function; the source does not provide evidence resolving the conjecture.

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Primary source

Si-Qi Liu, Di Yang, Youjin Zhang and Chunhui Zhou, “The Loop Equation for Special Cubic Hodge Integrals”, arXiv:1811.10234 (2020).

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