Affine meander-matrix conjecture for pure partition functions

Fix irrational κ(0,8)\kappa\in(0,8) and let LP(n,m)\mathrm{LP}(n,m) be the set of link patterns. Let Zα\mathcal{Z}_{\alpha} be the pure partition function indexed by αLP(n,m)\alpha\in\mathrm{LP}(n,m), and let Jα(m,n)\mathcal{J}^{(m,n)}_{\alpha} be the corresponding Coulomb gas integral. Let Mκ\mathcal{M}_{\kappa} denote the affine meander matrix. Affine meander-matrix conjecture. For every βLP(n,m)\beta\in\mathrm{LP}(n,m),

Jβ(m,n)(x)=αLP(n,m)Mκ(α,β)Zα(x),\mathcal{J}_\beta^{(m,n)}(\boldsymbol{x})=\sum_{\alpha\in\operatorname{LP}(n,m)}\mathcal{M}_{\kappa}(\alpha,\beta)\mathcal{Z}_\alpha(\boldsymbol{x}),

and conversely,

Zβ(x)=αLP(n,m)Mκ(α,β)1Jα(m,n)(x).\mathcal{Z}_\beta(\boldsymbol{x})=\sum_{\alpha\in\operatorname{LP}(n,m)}\mathcal{M}_{\kappa}(\alpha,\beta)^{-1}\mathcal{J}_\alpha^{(m,n)}(\boldsymbol{x}).

The relations identify the Coulomb gas integrals with the pure partition functions through the affine meander matrix; the supplied text gives no resolution or further evidence of their status.

Sources & referencesView supporting material

Primary source

Jiaxin Zhang, “Asymptotic of Coulomb gas integral, Temperley-Lieb type algebras and pure partition functions”, arXiv:2506.01306 (2025).

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