TY - JOUR
T1 - On-shell structures of MHV amplitudes beyond the planar limit
AU - Arkani-Hamed, Nima
AU - Bourjaily, Jacob L.
AU - Cachazo, Freddy
AU - Postnikov, Alexander
AU - Trnka, Jaroslav
N1 - Publisher Copyright:
© 2015, The Author(s).
PY - 2015/6/2
Y1 - 2015/6/2
N2 - Abstract: We initiate an exploration of on-shell functions in N=4$$ \mathcal{N}=4 $$ SYM beyond the planar limit by providing compact, combinatorial expressions for all leading singularities of MHV amplitudes and showing that they can always be expressed as a positive sum of differently ordered Parke-Taylor tree amplitudes. This is understood in terms of an extended notion of positivity in G(2, n), the Grassmannian of 2-planes in n dimensions: a single on-shell diagram can be associated with many different “positive” regions, of which the familiar G+(2, n) associated with planar diagrams is just one example. The decomposition into Parke-Taylor factors is simply a “triangulation” of these extended positive regions. The U(1) decoupling and Kleiss-Kuijf (KK) relations satisfied by the Parke-Taylor amplitudes also follow naturally from this geometric picture. These results suggest that non-planar MHV amplitudes in N=4$$ \mathcal{N}=4 $$ SYM at all loop orders can be expressed as a sum of polylogarithms weighted by color factors and (unordered) Parke-Taylor amplitudes.
AB - Abstract: We initiate an exploration of on-shell functions in N=4$$ \mathcal{N}=4 $$ SYM beyond the planar limit by providing compact, combinatorial expressions for all leading singularities of MHV amplitudes and showing that they can always be expressed as a positive sum of differently ordered Parke-Taylor tree amplitudes. This is understood in terms of an extended notion of positivity in G(2, n), the Grassmannian of 2-planes in n dimensions: a single on-shell diagram can be associated with many different “positive” regions, of which the familiar G+(2, n) associated with planar diagrams is just one example. The decomposition into Parke-Taylor factors is simply a “triangulation” of these extended positive regions. The U(1) decoupling and Kleiss-Kuijf (KK) relations satisfied by the Parke-Taylor amplitudes also follow naturally from this geometric picture. These results suggest that non-planar MHV amplitudes in N=4$$ \mathcal{N}=4 $$ SYM at all loop orders can be expressed as a sum of polylogarithms weighted by color factors and (unordered) Parke-Taylor amplitudes.
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U2 - 10.1007/JHEP06(2015)179
DO - 10.1007/JHEP06(2015)179
M3 - Article
AN - SCOPUS:84934293559
SN - 1126-6708
VL - 2015
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 6
M1 - 179
ER -