Scattering equations: from projective spaces to tropical grassmannians

Abstract We introduce a natural generalization of the scattering equations, which connect the space of Mandelstam invariants to that of points on ℂℙ1, to higher-dimensional projective spaces ℂℙk − 1. The standard, k = 2 Mandelstam invariants, sab, are generalized to completely symmetric tensors s a...

Full description

Bibliographic Details
Main Authors: Cachazo, Freddy (Author), Early, Nick (Author), Guevara, Alfredo (Author), Mizera, Sebastian (Author)
Format: Article
Language:English
Published: Springer Berlin Heidelberg, 2021-09-20T17:29:35Z.
Subjects:
Online Access:Get fulltext
LEADER 01600 am a22001693u 4500
001 131678
042 |a dc 
100 1 0 |a Cachazo, Freddy  |e author 
700 1 0 |a Early, Nick  |e author 
700 1 0 |a Guevara, Alfredo  |e author 
700 1 0 |a Mizera, Sebastian  |e author 
245 0 0 |a Scattering equations: from projective spaces to tropical grassmannians 
260 |b Springer Berlin Heidelberg,   |c 2021-09-20T17:29:35Z. 
856 |z Get fulltext  |u https://hdl.handle.net/1721.1/131678 
520 |a Abstract We introduce a natural generalization of the scattering equations, which connect the space of Mandelstam invariants to that of points on ℂℙ1, to higher-dimensional projective spaces ℂℙk − 1. The standard, k = 2 Mandelstam invariants, sab, are generalized to completely symmetric tensors s a 1 a 2 ... a k $$ {\mathrm{s}}_{a_1{a}_2\dots {a}_k} $$ subject to a 'massless' condition s a 1 a 2 ... a k − 2 b b = 0 $$ {\mathrm{s}}_{a_1{a}_2\dots {a}_{k-2}bb}=0 $$ and to 'momentum conservation'. The scattering equations are obtained by constructing a potential function and computing its critical points. We mainly concentrate on the k = 3 case: study solutions and define the generalization of biadjoint scalar amplitudes. We compute all 'biadjoint amplitudes' for (k, n) = (3, 6) and find a direct connection to the tropical Grassmannian. This leads to the notion of k = 3 Feynman diagrams. We also find a concrete realization of the new kinematic spaces, which coincides with the spinor-helicity formalism for k = 2, and provides analytic solutions analogous to the MHV ones. 
546 |a en 
655 7 |a Article