2016
DOI: 10.1007/jhep12(2016)076
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Grassmannians and form factors with q 2 = 0 in N $$ \mathcal{N} $$ =4 SYM theory

Abstract: In this paper we consider tree level form factors of operators from stress tensor operator supermultiplet with light-like operator momentum q 2 = 0. We present a conjecture for the Grassmannian integral representation both for these tree level form factors as well as for leading singularities of their loop counterparts. The presented conjecture was successfully checked by reproducing several known answers in MHV and N k−2 MHV, k ≥ 3 sectors together with appropriate soft limits. We also discuss the cancellatio… Show more

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Cited by 15 publications
(8 citation statements)
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“…Form factors of half-BPS operator are by now very well studied, both at weak [17][18][19][20][21][22][23][24][25][26] and strong coupling [27,28]. The extension to form factors of the on-shell diagram formalism and their formulation in terms of twistor variables, exhibiting an underlying Graßmannian geometry, have also been studied [29][30][31][32][33][34][35]. Yet, despite the availability of many perturbative results, the dual conformal symmetry properties of form factors of protected operators have not yet been investigated (see [36] for comments regarding the q 2 = 0 case).…”
Section: Introductionmentioning
confidence: 99%
“…Form factors of half-BPS operator are by now very well studied, both at weak [17][18][19][20][21][22][23][24][25][26] and strong coupling [27,28]. The extension to form factors of the on-shell diagram formalism and their formulation in terms of twistor variables, exhibiting an underlying Graßmannian geometry, have also been studied [29][30][31][32][33][34][35]. Yet, despite the availability of many perturbative results, the dual conformal symmetry properties of form factors of protected operators have not yet been investigated (see [36] for comments regarding the q 2 = 0 case).…”
Section: Introductionmentioning
confidence: 99%
“…Now we should recall that the Wilson lines were used here to describe scattering of two fast moving particles at high energy. 23 This restricts further our kinematics, so that p 1 ·p 2 = s/2 (s is the usual Mandelstam variable) and momentum transfer between two particles is restricted by two orthogonality conditions k · p 1 = k · p 2 = 0. The latter two conditions allow us to write down transverse momentum transfer as…”
Section: Virtual Part Of Lo Bfklmentioning
confidence: 99%
“…Color-kinematics duality has been applied to compute form factors in [50,51]. Grassmannian and polytopes pictures were studied in [52,53,54,55,56]. The twistor formalism was applied to form factors in [57,58,59,60].…”
Section: Introductionmentioning
confidence: 99%