The tau-function as conformal block conjecture for W(sl_d)-symmetric Toda theories

Let MW(sld)P1\mathcal M_{\mathcal W({\mathfrak{sl}_d})}^{\mathbb P^1} be the moduli space of marked points, weights, and times, and let Tz,α,t\mathfrak T_{\bold z,\bold \alpha,\bold t} be the tau-function defined by

lnTz,α,t=g=0ε2g2Fg.\ln\mathfrak T_{\bold z,\bold \alpha,\bold t}=\sum_{g=0}^{\infty}\varepsilon^{2g-2}\mathcal F_g.

Here z=(z1,,zM)\bold z=(z_1,\ldots,z_M) and α=(α1,,αM)\boldsymbol\alpha=(\alpha_1,\ldots,\alpha_M) specify the insertions Vαj(zj)V_{\alpha_j}(z_j) in the associated W(sld)\mathcal W(\mathfrak{sl}_d)-symmetric conformal field theory. Tau-function as conformal block conjecture. The tau-function equals the conformal block

Tz,α,t=j=1MVαj(zj).\mathfrak T_{\bold z,\bold \alpha,\bold t}=\left\langle\prod_{j=1}^{M}V_{\alpha_j}(z_j)\right\rangle.

The conjecture identifies the integrable-system tau-function constructed from the special-geometry data with the conformal-field-theory correlation function. The paper presents this as a natural conjecture; no resolution is supplied in the given text.

Sources & referencesView supporting material

Primary source

Raphaël Belliard and Bertrand Eynard, “Integrability of W(sl_d)-symmetric Toda conformal field theories I : Quantum geometry”, arXiv:1801.03433 (2019).

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