2005
DOI: 10.1016/j.nuclphysb.2005.02.030
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New recursion relations for tree amplitudes of gluons

Abstract: We present new recursion relations for tree amplitudes in gauge theory that give very compact formulas. Our relations give any tree amplitude as a sum over terms constructed from products of two amplitudes of fewer particles multiplied by a Feynman propagator.The two amplitudes in each term are physical, in the sense that all particles are on-shell and momentum conservation is preserved. This is striking, since it is just like adding certain factorization limits of the original amplitude to build up the full a… Show more

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Cited by 1,026 publications
(1,965 citation statements)
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References 28 publications
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“…More recently, a new set of recursion relations for tree level amplitudes of gluons was introduced by Britto, Feng and the third author [7]. These recursion relations were inspired by [8,9] and reproduced very compact results obtained in [10] by studying the IR behavior of N = 4 one-loop amplitudes.…”
Section: Introductionmentioning
confidence: 89%
See 1 more Smart Citation
“…More recently, a new set of recursion relations for tree level amplitudes of gluons was introduced by Britto, Feng and the third author [7]. These recursion relations were inspired by [8,9] and reproduced very compact results obtained in [10] by studying the IR behavior of N = 4 one-loop amplitudes.…”
Section: Introductionmentioning
confidence: 89%
“…One in which an amplitude is given as a sum of terms containing the product of two physical on-shell amplitudes where the momenta of only two gravitons have been complexified. These recursion relations, originally discovered in [7] in gauge theory, were proven using the power of complex analysis in [11]. The BCFW construction opened up the possibility for using complex analysis in many other situations.…”
Section: Conclusion and Further Directionsmentioning
confidence: 95%
“…In particular, the supersymmetric Ward identities determine in these four dimensions [19] A(+ + · · · +) = 0 , 12) with an exception only for the three particle A(+ + −) and A(− − +) amplitude which vanish generically only for all momenta in R (1,3) . The input in this argument is nothing more than simple representation theory of on-shell N = 1 space-time supersymmetry and the absence of helicity-violating fermion amplitudes.…”
Section: Effective Supersymmetrymentioning
confidence: 99%
“…In an alternate approach to computing tree level amplitudes, Britto, Cachazo, Feng and Witten [17] obtained a recursion relation based on analytically shifting a pair of external legs, λ i −→ λ i + zλ j ,λ j −→λ j − zλ i , (1.4) and determining the physical amplitude, A n (0), from the poles in the shifted amplitude, A n (z). This leads to a recursion relation in the number of external legs, n, of the form, 5) where the factorisation is only on these poles, z α , where legs i and j are connected to different sub-amplitudes.…”
Section: Introductionmentioning
confidence: 99%