The octagon equation of the non-compact quantum dilogarithm

Let PP, QQ, and VV be as in Lem.. The octagon equation of the non-compact quantum dilogarithm.

Φ3(3P)Φ(Q)=Φ(Q)Φ3(3P+3Q)Φ(3P+2Q)Φ3(6P+3Q)Φ(3P+Q)Φ3(3P).\Phi^{3\hbar}(3P) \Phi^\hbar(Q) = \Phi^\hbar(Q) \Phi^{3\hbar}(3P+3Q) \Phi^\hbar(3P+2Q) \Phi^{3\hbar}(6P+3Q) \Phi^\hbar(3P+Q) \Phi^{3\hbar}(3P).

This identity is presented as the equation corresponding to Fock–Goncharov's G2G_2-type operator identity and is introduced after a heuristic discussion of related quantum dilogarithm identities. The supplied text does not establish whether the equation has been proved in full generality.

Equivalent formulations 1

Other statements of this same problem, merged from separate entries. Each is equivalent to the statement above — proving any one settles them all.

  1. The octagon equation of the non-compact quantum dilogarithm

    Let PP, QQ, and VV be as in Lemma cited in the source. The octagon equation.

    Φ3(3P)Φ(Q)=Φ(Q)Φ3(3P+3Q)Φ(3P+2Q)Φ3(6P+3Q)Φ(3P+Q)Φ3(3P).\Phi^{3\hbar}(3P)\Phi^\hbar(Q)=\Phi^\hbar(Q)\Phi^{3\hbar}(3P+3Q)\Phi^\hbar(3P+2Q)\Phi^{3\hbar}(6P+3Q)\Phi^\hbar(3P+Q)\Phi^{3\hbar}(3P).

    This identity is the operator relation corresponding to Fock–Goncharov's G2G_2-type identity; the supplied text presents it as a suggested relation in a heuristic discussion, without establishing its resolution here.

    source: Hyun Kyu Kim, “Phase constants in the Fock-Goncharov quantization of cluster varieties: long version”, arXiv:1602.00361 (2016).

Sources & referencesView supporting material

Primary source

Hyun Kyu Kim, “Phase constants in the Fock-Goncharov quantum cluster varieties”, arXiv:1602.00797 (2019).

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