PreprintarXiv licencearXiv
From amplituhedra to flagtopes
Abstract
The amplituhedron was introduced by Arkani-Hamed and Trnka (2014) to geometrically encode scattering amplitudes in high-energy physics. It can be viewed as the generalization of a cyclic polytope into the Grassmannian, and is defined to be the projection of the totally nonnegative part of one Grassmannian with respect to a totally negative element of a second Grassmannian. We construct a Lie-theoretic generalization of amplituhedra called 'flag amplituhedra', by replacing the pair of Grassmannians in the definition with an arbitrary pair of partial flag varieties for a reductive group G. We study in detail an example of a flag amplituhedron which is not a Grassmannian amplituhedron; it is a curved hexagon in ℙ1× ℙ1.
Related
BibTeX
@misc{barkley2026from,
title = {{From amplituhedra to flagtopes}},
author = {Grant T. Barkley and Steven N. Karp and Kaitao Xie},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.37017},
eprint = {2610.37017},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.37017},
}
RIS
TY - UNPB
TI - From amplituhedra to flagtopes
AU - Grant T. Barkley
AU - Steven N. Karp
AU - Kaitao Xie
PY - 2026
DA - 2026/10/27
PB - arXiv
DO - 10.48550/arxiv.2610.37017
UR - https://arxiv.org/abs/2610.37017
AB - The amplituhedron was introduced by Arkani-Hamed and Trnka (2014) to geometrically encode scattering amplitudes in high-energy physics. It can be viewed as the generalization of a cyclic polytope into the Grassmannian, and is defined to be the projection of the totally nonnegative part of one Grassmannian with respect to a totally negative element of a second Grassmannian. We construct a Lie-theoretic generalization of amplituhedra called 'flag amplituhedra', by replacing the pair of Grassmannians in the definition with an arbitrary pair of partial flag varieties for a reductive group G. We study in detail an example of a flag amplituhedron which is not a Grassmannian amplituhedron; it is a curved hexagon in ℙ^1× ℙ^1.
ER -