Constraints and Generalized Gauge Transformations on Tree-Level Gluon and Graviton Amplitudes

preprint2010arXivOpen access

Abstract

Writing the fully color dressed and graviton amplitudes, respectively, as A=<C∣A>=<C∣M∣N>{\bf A}=<C|A> =<C|M|N> and Agr=<N~∣M∣N>{\bf A}_{gr}= <\tilde N|M|N> , where ∣A>|A> is a set of Kleiss-Kuijf color-ordered basis, ∣N>,|N>, |\tilde N> and and |C>arethesimilarlyorderednumeratorsandcolorcoefficients,weshowthatthepropagatormatrix are the similarly ordered numerators and color coefficients, we show that the propagator matrix Mhas has (n-3)(n-3)!independenteigenvectors independent eigenvectors |λ^0_j>withzeroeigenvalue,for with zero eigenvalue, for n−particleprocesses.Theresultingequations-particle processes. The resulting equations <λ^0_j|A> = 0arerelationsamongthecolororderedamplitudes.Thefreedomtoshift are relations among the color ordered amplitudes. The freedom to shift |N> \to |N> +\sum_j f_j|λ^0_j>andsimilarlyfor and similarly for |\tilde N>,where, where f_jare are (n-3)(n-3)!arbitraryfunctions,encodesgeneralizedgaugetransformations.TheyyieldbothBCJamplitudeandKLTrelations,whensuchfreedomisaccountedfor.Furthermore, arbitrary functions, encodes generalized gauge transformations. They yield both BCJ amplitude and KLT relations, when such freedom is accounted for. Furthermore, f_j$ can be promoted to the role of effective Lagrangian vertices in the field operator space.

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