Résumé
The computation of a certain class of four-point functions of heavily charged BPS operators boils down to the computation of a special form factor — the octagon. In this paper, which is an extended version of the short note [1], we derive a non-perturbative formula for the square of the octagon as the determinant of a semi-infinite skew-symmetric matrix. We show that perturbatively in the weak coupling limit the octagon is given by a determinant constructed from the polylogarithms evaluating ladder Feynman graphs. We also give a simple operator representation of the octagon in terms of a vacuum expectation value of massless free bosons or fermions living in the rapidity plane.
| langue originale | Anglais |
|---|---|
| Numéro d'article | 178 |
| journal | Journal of High Energy Physics |
| Volume | 2019 |
| Numéro de publication | 11 |
| Les DOIs | |
| état | Publié - 1 nov. 2019 |
| Modification externe | Oui |
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