The scalar proportionality conjecture for the qKZB heat kernel

From papers

Let U(z,τ,p)U({\vec{z}},\tau,p) be the function defined in Corollary 1, namely

U(z,τ,p)=αQτ+pα(u(z,τ,τ+p)u(z,τ+p,p)).U({\vec{z}},\tau,p)=\alpha\otimes Q_{\tau+p}\otimes\alpha\bigl(u({\vec{z}},\tau,\tau+p)\otimes u({\vec{z}},\tau+p,p)\bigr).

Here uu is the function appearing in the qKZB heat equation, α\alpha is multiplication by the function α(λ)\alpha(\lambda), and Qτ+pQ_{\tau+p} is the operator introduced in the definition of the heat operator. Scalar proportionality conjecture. There is a constant CC such that

U(z,τ,p)=Cu(z,τ,p).U({\vec{z}},\tau,p)=C u({\vec{z}},\tau,p).

This asserts that the composition of the two qKZB heat kernels is proportional to the single heat kernel with combined parameters. The supplied text does not state whether the claim has been proved or disproved.

Progress summary

Nothing recorded yet. Refresh searches the literature and the public web for attempts on this problem, and writes the first summary here.

Sources & referencesView supporting material

Primary source

Giovanni Felder and Alexander Varchenko, “The q-deformed Knizhnik-Zamolodchikov-Bernard heat equation”, arXiv:math/9809139 (2000).

Solutions 0

No solutions have been posted yet.