Abstract:Abstract:The subleading corrections to factorization theorems for soft bremsstrahlung in nonabelian gauge theories and gravity are investigated in the case of a five point amplitude with four scalars. Building on recent results, we write the action of the angular momentum operators on scattering amplitudes as derivatives with respect to the Mandelstam invariants to uncover a double copy structure in the contribution of the soft graviton to the amplitude, both in the leading term and the first correction. Using… Show more
“…This double copy structure has a historic antecedent in the Kawai, Lewellen, and Tye (KLT) relations [4], showing how, at tree level, closed string amplitudes admit a decomposition in terms of products of open string amplitudes. Similar structures have been found in various other setups [5][6][7]. It seems clear that, at the level of scattering amplitudes, there is a sense in which gravity can be considered the "square" of a gauge theory.…”
Section: Introductionsupporting
confidence: 78%
“…, 8) or (21,22,23) we recover previous examples. For instance, (a 1 , a 2 , a 3 , a 4 , a 5 ) = (7,7,6,1,5) gives the curve shown in the l.h.s. panel of figure 4, whereas (a 1 , a 2 , a 3 , a 4 , a 5 ) = (22,23,21,21,21) reproduces eq.…”
Planar zeros are studied in the context of the five-point scattering amplitude for gauge bosons and gravitons. In the case of gauge theories, it is found that planar zeros are determined by an algebraic curve in the projective plane spanned by the three stereographic coordinates labelling the direction of the outgoing momenta. This curve depends on the values of six independent color structures. Considering the gauge group SU(N ) with N = 2, 3, 5 and fixed color indices, the class of curves obtained gets broader by increasing the rank of the group. For the five-graviton scattering, on the other hand, we show that the amplitude vanishes whenever the process is planar, without imposing further kinematic conditions. A rationale for this result is provided using color-kinematics duality.
“…This double copy structure has a historic antecedent in the Kawai, Lewellen, and Tye (KLT) relations [4], showing how, at tree level, closed string amplitudes admit a decomposition in terms of products of open string amplitudes. Similar structures have been found in various other setups [5][6][7]. It seems clear that, at the level of scattering amplitudes, there is a sense in which gravity can be considered the "square" of a gauge theory.…”
Section: Introductionsupporting
confidence: 78%
“…, 8) or (21,22,23) we recover previous examples. For instance, (a 1 , a 2 , a 3 , a 4 , a 5 ) = (7,7,6,1,5) gives the curve shown in the l.h.s. panel of figure 4, whereas (a 1 , a 2 , a 3 , a 4 , a 5 ) = (22,23,21,21,21) reproduces eq.…”
Planar zeros are studied in the context of the five-point scattering amplitude for gauge bosons and gravitons. In the case of gauge theories, it is found that planar zeros are determined by an algebraic curve in the projective plane spanned by the three stereographic coordinates labelling the direction of the outgoing momenta. This curve depends on the values of six independent color structures. Considering the gauge group SU(N ) with N = 2, 3, 5 and fixed color indices, the class of curves obtained gets broader by increasing the rank of the group. For the five-graviton scattering, on the other hand, we show that the amplitude vanishes whenever the process is planar, without imposing further kinematic conditions. A rationale for this result is provided using color-kinematics duality.
“…This exhibits the double-copy structure of graviton amplitudes, already found in many other physical setups [30][31][32][33][34][35]. Similarly, biadjoint scalar amplitudes can be obtained from eq.…”
Section: Scattering Amplitudessupporting
confidence: 66%
“…The connection among gravitational and Yang-Mills amplitudes in this approach from the point of view of Regge kinematics [40][41][42][43] is also of interest, together with the corresponding soft theorems [35,[44][45][46][47][48]. Besides, it would be interesting to interpret the role of the gluing operator recently investigated in [37] in terms of Sudakov variables.…”
Section: Jhep01(2018)057 6 Conclusion and Outlookmentioning
Abstract:We show that the use of Sudakov variables greatly simplifies the study of the solutions to the scattering equations in the Cachazo-He-Yuan formalism. We work in the center-of-mass frame for the two incoming particles, which partially fixes the SL(2, C) redundancy in the integrand defining the scattering amplitudes, the remaining freedom translates into a global shift in the azimuthal angle of the outgoing particles. Studying four-and five-particle amplitudes, we see how an appropriate choice of this phase allows for algebraic simplifications when finding solutions to the scattering equations, as well as in the expression of the scattering amplitudes in terms of the locations of the punctures in the sphere. These punctures themselves are remarkably simple functions of the Sudakov parameters.
“…In the limit in which the emitted positive (resp. negative) helicity gluon is soft, p 5 → 0, the leading behavior of the amplitude takes the form [40] A 5,soft = 2g…”
Section: Jhep05(2017)011 7 Remarks On Soft Limitsmentioning
Abstract:We study the projective properties of planar zeros of tree-level scattering amplitudes in various theories. Whereas for pure scalar field theories we find that the planar zeros of the five-point amplitude do not enjoy projective invariance, coupling scalars to gauge fields gives rise to tree-level amplitudes whose planar zeros are determined by homogeneous polynomials in the stereographic coordinates labelling the direction of flight of the outgoing particles. In the case of pure gauge theories, this projective structure is generically destroyed if string corrections are taken into account. Scattering amplitudes of two scalars with graviton emission vanish exactly in the planar limit, whereas planar graviton amplitudes are zero for helicity violating configurations. These results are corrected by string effects, computed using the single-valued projection, which render the planar amplitude nonzero. Finally, we discuss how the structure of planar zeros can be derived from the soft limit behavior of the scattering amplitudes.
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