Motivic Gerasimov–Shatashvili amplitude conjecture

Let AQp(N)(s)A_{\mathbb{Q}_p}^{(N)}(\boldsymbol{s}) be the pp-adic Koba–Nielsen amplitudes, and let AC((T))(N)(L)A_{\mathbb{C((}T\mathbb{))}}^{(N)}(\boldsymbol{L}) denote the motivic string amplitudes over C((T))\mathbb{C((}T\mathbb{))}. Their specialization at L=p\boldsymbol{L}=p gives the pp-adic amplitudes, while specialization at L=1\boldsymbol{L}=1 gives the Denef–Loeser amplitudes. Let AGS(N)A_{GS}^{(N)} denote the Feynman amplitudes of the Gerasimov–Shatashvili Lagrangian at the motivic, or “three”, level. Motivic Gerasimov–Shatashvili conjecture. The Feynman amplitudes at the three level of the Gerasimov–Shatashvili Lagrangian are related to

limp1AQp(N)(s).\lim_{p\rightarrow1}A_{\mathbb{Q}_p}^{(N)}(\boldsymbol{s}).

The paper reports verification for the four- and five-point amplitudes, while the general statement remains conjectural; the wording “are by related” is reproduced mathematically as an unspecified relation.

Sources & referencesView supporting material

Primary source

M. Bocardo-Gaspar, H. García-Compeán, Edgar Y. López and W. A. Zúñiga-Galindo, “Local Zeta Functions and Koba-Nielsen String Amplitudes”, arXiv:2105.00298 (2021).

Progress summary

Never refreshed

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

Solutions 0

No solutions have been posted yet.