The pentagon relation for Baxter operators in the punctured-torus skein algebra

Let T2DT^2-D be the once-punctured torus, and let Sk^(T2D)\widehat{\operatorname{Sk}}(T^2-D) be its completed skein algebra. For x,yZ2\mathbf{x},\mathbf{y}\in\mathbb{Z}^2, let ω(x,y)\omega(\mathbf{x},\mathbf{y}) denote their intersection pairing, and let Qx(v)Q_{\mathbf{x}}(v) and Qy(w)Q_{\mathbf{y}}(w) be the corresponding Baxter operators. Pentagon relation. If

ω(x,y)=1,\omega(\mathbf{x},\mathbf{y})=1,

then

Qx(v)Qy(w)=Qy(w)Qx+y(vw)Qx(v)Q_{\mathbf{x}}(v)\cdot Q_{\mathbf{y}}(w)=Q_{\mathbf{y}}(w)\cdot Q_{\mathbf{x}+\mathbf{y}}(vw)\cdot Q_{\mathbf{x}}(v)

in Sk^(T2D)\widehat{\operatorname{Sk}}(T^2-D). This is the punctured-torus analogue of the Baxter pentagon relation established for the closed torus in the preceding theorem; the source provides the relation as a conjectural statement, and its resolution is not indicated here.

Sources & referencesView supporting material

Primary source

Mingyuan Hu, Gus Schrader and Eric Zaslow, “Skeins, clusters and wavefunctions”, arXiv:2312.10186 (2023).

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