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The momentum amplituhedron of SYM and ABJM from twistor-string maps
We study remarkable connections between twistor-string formulas for tree amplitudes in \({\cal N}=4\) SYM and \({\cal N}=6\) ABJM, and the corresponding momentum amplituhedron in the kinematic space of \(D=4\) and \(D=3\), respectively. Based on the Veronese map to positive Grassmannians, we define...
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Published in: | arXiv.org 2022-04 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | We study remarkable connections between twistor-string formulas for tree amplitudes in \({\cal N}=4\) SYM and \({\cal N}=6\) ABJM, and the corresponding momentum amplituhedron in the kinematic space of \(D=4\) and \(D=3\), respectively. Based on the Veronese map to positive Grassmannians, we define a twistor-string map from \(G_{+}(2,n)\) to a \((2n{-}4)\)-dimensional subspace of the 4d kinematic space where the momentum amplituhedron of SYM lives. We provide strong evidence that the twistor-string map is a diffeomorphism from \(G_+(2,n)\) to the interior of momentum amplituhedron; the canonical form of the latter, which is known to give tree amplitudes of SYM, can be obtained as pushforward of that of former. We then move to three dimensions: based on Veronese map to orthogonal positive Grassmannian, we propose a similar twistor-string map from the moduli space \({\cal M}_{0,n}^+\) to a \((n{-}3)\)-dimensional subspace of 3d kinematic space. The image gives a new positive geometry which conjecturally serves as the momentum amplituhedron for ABJM; its canonical form gives the tree amplitude with reduced supersymmetries in the theory. We also show how boundaries of compactified \({\cal M}_{0,n}^+\) map to boundaries of momentum amplituhedra for SYM and ABJM corresponding to factorization channels of amplitudes, and in particular for ABJM case the map beautifully excludes all unwanted channels. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.2111.02576 |