Abstract:Abstract:We investigate the existence of relations for finite one-loop amplitudes in YangMills theory. Using a diagrammatic formalism and a remarkable connection between tree and loop level, we deduce sequences of amplitude relations for any number of external legs.
“…(1.2) This duality between the color and kinematic factors was later found to be present in a variety of Yang-Mills theories [2][3][4][5][6][7][8][9][10] and, perhaps most surprisingly, was shown to be valid at least for the first few loop levels [2,3,[5][6][7][8][9][11][12][13][14][15][16][17][18][19]. The apparently symmetrical structure also suggests mirror versions of the existing color decomposition formulations.…”
Section: Introductionmentioning
confidence: 85%
“…, n − 1) by construction. Since all permutations can be generated by successive permutations between the (n − 1) consequtive pairs, we can reduce our checking to the following two permutations: (12) and (n − 1)n. Now let us consider the numerators of dual-DDM form n 213...(n−1)n and n 123...n(n−1) . We have two ways to get the same n α from basis numerators: one is by relabeling n 123...(n−1)n and another one, by using Jacobi relation and antisymmetry.…”
We present an algorithm that leads to BCJ numerators satisfying manifestly the three properties proposed by Broedel and Carrasco in [42]. We explicitly calculate the numerators at 4, 5 and 6-points and show that the relabeling property is generically satisfied.
“…(1.2) This duality between the color and kinematic factors was later found to be present in a variety of Yang-Mills theories [2][3][4][5][6][7][8][9][10] and, perhaps most surprisingly, was shown to be valid at least for the first few loop levels [2,3,[5][6][7][8][9][11][12][13][14][15][16][17][18][19]. The apparently symmetrical structure also suggests mirror versions of the existing color decomposition formulations.…”
Section: Introductionmentioning
confidence: 85%
“…, n − 1) by construction. Since all permutations can be generated by successive permutations between the (n − 1) consequtive pairs, we can reduce our checking to the following two permutations: (12) and (n − 1)n. Now let us consider the numerators of dual-DDM form n 213...(n−1)n and n 123...n(n−1) . We have two ways to get the same n α from basis numerators: one is by relabeling n 123...(n−1)n and another one, by using Jacobi relation and antisymmetry.…”
We present an algorithm that leads to BCJ numerators satisfying manifestly the three properties proposed by Broedel and Carrasco in [42]. We explicitly calculate the numerators at 4, 5 and 6-points and show that the relabeling property is generically satisfied.
“…The "KK-like" relations among the ζ 2 -orders of open superstring amplitudes [112,117,118] for instance are known to annihilate permutation sums at multiplicities n ≥ 5 and therefore…”
Section: Selection Rule For the First Order In ζmentioning
In this paper we derive the tree-level S-matrix of the effective theory of Goldstone bosons known as the non-linear sigma model (NLSM) from string theory. This novel connection relies on a recent realization of tree-level open-superstring S-matrix predictions as a double copy of super-Yang-Mills theory with Z-theory -the collection of putative scalar effective field theories encoding all the α ′ -expansion of the open superstring. Here we identify the color-ordered amplitudes of the NLSM as the low-energy limit of abelian Z-theory. This realization also provides natural higher-derivative corrections to the NLSM amplitudes arising from higher powers of α ′ in the abelian Z-theory amplitudes, and through double copy also to Born-Infeld and Volkov-Akulov theories. The amplitude relations due to Kleiss-Kuijf as well as Bern, Johansson and one of the current authors obeyed by Z-theory amplitudes thereby apply to all α ′ -corrections of the NLSM. As such we naturally obtain a cubic-graph parameterization for the abelian Z-theory predictions whose kinematic numerators obey the duality between color and kinematics to all orders in α ′ .
Color-ordered amplitudes for the scattering of n particles in the adjoint representation of SU(N ) gauge theory satisfy constraints that arise from group theory alone. These constraints break into subsets associated with irreducible representations of the symmetric group S n , which allows them to be presented in a compact and natural way. Using an iterative approach, we derive the constraints for six-point amplitudes at all loop orders, extending earlier results for n = 4 and n = 5. We then decompose the four-, five-, and six-point group-theory constraints into their irreducible S n subspaces. We comment briefly on higher-point two-loop amplitudes.
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