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Scattering amplitudes and the positive Grassmannian
We establish a direct connection between scattering amplitudes in planar four-dimensional theories and a remarkable mathematical structure known as the positive Grassmannian. The central physical idea is to focus on on-shell diagrams as objects of fundamental importance to scattering amplitudes. We...
Autores principales: | , , , , , |
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Lenguaje: | eng |
Publicado: |
2012
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Acceso en línea: | http://cds.cern.ch/record/1502539 |
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author | Arkani-Hamed, Nima Bourjaily, Jacob L Cachazo, Freddy Goncharov, Alexander B Postnikov, Alexander Trnka, Jaroslav |
author_facet | Arkani-Hamed, Nima Bourjaily, Jacob L Cachazo, Freddy Goncharov, Alexander B Postnikov, Alexander Trnka, Jaroslav |
author_sort | Arkani-Hamed, Nima |
collection | CERN |
description | We establish a direct connection between scattering amplitudes in planar four-dimensional theories and a remarkable mathematical structure known as the positive Grassmannian. The central physical idea is to focus on on-shell diagrams as objects of fundamental importance to scattering amplitudes. We show that the all-loop integrand in N=4 SYM is naturally represented in this way. On-shell diagrams in this theory are intimately tied to a variety of mathematical objects, ranging from a new graphical representation of permutations to a beautiful stratification of the Grassmannian G(k,n) which generalizes the notion of a simplex in projective space. All physically important operations involving on-shell diagrams map to canonical operations on permutations; in particular, BCFW deformations correspond to adjacent transpositions. Each cell of the positive Grassmannian is naturally endowed with positive coordinates and an invariant measure which determines the on-shell function associated with the diagram. This understanding allows us to classify and compute all on-shell diagrams, and give a geometric understanding for all the non-trivial relations among them. Yangian invariance of scattering amplitudes is transparently represented by diffeomorphisms of G(k,n) which preserve the positive structure. Scattering amplitudes in (1+1)-dimensional integrable systems and the ABJM theory in (2+1) dimensions can both be understood as special cases of these ideas. On-shell diagrams in theories with less (or no) supersymmetry are associated with exactly the same structures in the Grassmannian, but with a measure deformed by a factor encoding ultraviolet singularities. The Grassmannian representation of on-shell processes also gives a new understanding of the all-loop integrand for scattering amplitudes, presenting all integrands in a novel dLog form which directly reflects the underlying positive structure. |
id | cern-1502539 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2012 |
record_format | invenio |
spelling | cern-15025392021-04-21T23:55:00Zhttp://cds.cern.ch/record/1502539engArkani-Hamed, NimaBourjaily, Jacob LCachazo, FreddyGoncharov, Alexander BPostnikov, AlexanderTrnka, JaroslavScattering amplitudes and the positive GrassmannianParticle Physics - TheoryWe establish a direct connection between scattering amplitudes in planar four-dimensional theories and a remarkable mathematical structure known as the positive Grassmannian. The central physical idea is to focus on on-shell diagrams as objects of fundamental importance to scattering amplitudes. We show that the all-loop integrand in N=4 SYM is naturally represented in this way. On-shell diagrams in this theory are intimately tied to a variety of mathematical objects, ranging from a new graphical representation of permutations to a beautiful stratification of the Grassmannian G(k,n) which generalizes the notion of a simplex in projective space. All physically important operations involving on-shell diagrams map to canonical operations on permutations; in particular, BCFW deformations correspond to adjacent transpositions. Each cell of the positive Grassmannian is naturally endowed with positive coordinates and an invariant measure which determines the on-shell function associated with the diagram. This understanding allows us to classify and compute all on-shell diagrams, and give a geometric understanding for all the non-trivial relations among them. Yangian invariance of scattering amplitudes is transparently represented by diffeomorphisms of G(k,n) which preserve the positive structure. Scattering amplitudes in (1+1)-dimensional integrable systems and the ABJM theory in (2+1) dimensions can both be understood as special cases of these ideas. On-shell diagrams in theories with less (or no) supersymmetry are associated with exactly the same structures in the Grassmannian, but with a measure deformed by a factor encoding ultraviolet singularities. The Grassmannian representation of on-shell processes also gives a new understanding of the all-loop integrand for scattering amplitudes, presenting all integrands in a novel dLog form which directly reflects the underlying positive structure.arXiv:1212.5605oai:cds.cern.ch:15025392012-12-27 |
spellingShingle | Particle Physics - Theory Arkani-Hamed, Nima Bourjaily, Jacob L Cachazo, Freddy Goncharov, Alexander B Postnikov, Alexander Trnka, Jaroslav Scattering amplitudes and the positive Grassmannian |
title | Scattering amplitudes and the positive Grassmannian |
title_full | Scattering amplitudes and the positive Grassmannian |
title_fullStr | Scattering amplitudes and the positive Grassmannian |
title_full_unstemmed | Scattering amplitudes and the positive Grassmannian |
title_short | Scattering amplitudes and the positive Grassmannian |
title_sort | scattering amplitudes and the positive grassmannian |
topic | Particle Physics - Theory |
url | http://cds.cern.ch/record/1502539 |
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