2016
DOI: 10.1007/jhep01(2016)170
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Color-kinematics duality for QCD amplitudes

Abstract: We show that color-kinematics duality is present in tree-level amplitudes of quantum chromodynamics with massive flavored quarks. Starting with the color structure of QCD, we work out a new color decomposition for n-point tree amplitudes in a reduced basis of primitive amplitudes. These primitives, with k quark-antiquark pairs and (n − 2k) gluons, are taken in the (n − 2)!/k! Melia basis, and are independent under the color-algebra Kleiss-Kuijf relations. This generalizes the color decomposition of Del Duca, D… Show more

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Cited by 163 publications
(312 citation statements)
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References 172 publications
(359 reference statements)
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“…We will use this freedom to fix a particle at position 1 and a second particle at position n. Since we also assume that there is at least one gluon, let us label this gluon by 2 g . In [14] Johansson and Ochirov conjecture that which follows from eq. (2.6) by momentum conservation.…”
Section: Jhep09(2015)197mentioning
confidence: 97%
“…We will use this freedom to fix a particle at position 1 and a second particle at position n. Since we also assume that there is at least one gluon, let us label this gluon by 2 g . In [14] Johansson and Ochirov conjecture that which follows from eq. (2.6) by momentum conservation.…”
Section: Jhep09(2015)197mentioning
confidence: 97%
“…In this construction the duality (2.2) needs to be manifest in only one of the two gauge theories [25,49]. This construction also extends to cases where the gauge theory includes fundamental-representation matter particles [50,51].…”
Section: Absence Of Enhanced Cancellations In the Integrandmentioning
confidence: 99%
“…More generally, once we have two gauge theories (with matter interactions or supersymmetry extension) that both can satisfy the color-kinematic duality, double copy constructions will always lead to gravity scattering amplitudes [7,[18][19][20][21][22][23].…”
Section: Jhep04(2017)033mentioning
confidence: 99%
“…For a given tree, we replace the end points of each path by k, and the internal vertices by k µ k ν . For example, we have: 18) where V 1 = 1, and V 2 can be either the root 1, or one of the φ(i)'s. 9 Finally, n NLSM (1, β β β, n) is obtained by summing up all these contributing trees.…”
Section: Jhep04(2017)033mentioning
confidence: 99%