English

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

High Energy Physics - Theory 2010-11-11 v2

Abstract

Writing the fully color dressed and graviton amplitudes, respectively, as A=<CA>=<CMN>{\bf A}=<C|A> =<C|M|N> and Agr=<N~MN>{\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 |\lambda ^0_j>withzeroeigenvalue,for with zero eigenvalue, for nparticleprocesses.Theresultingequations-particle processes. The resulting equations <\lambda ^0_j|A> = 0arerelationsamongthecolororderedamplitudes.Thefreedomtoshift are relations among the color ordered amplitudes. The freedom to shift |N> \to |N> +\sum_j f_j|\lambda ^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.

Keywords

Cite

@article{arxiv.1007.3475,
  title  = {Constraints and Generalized Gauge Transformations on Tree-Level Gluon and Graviton Amplitudes},
  author = {Diana Vaman and York-Peng Yao},
  journal= {arXiv preprint arXiv:1007.3475},
  year   = {2010}
}

Comments

22 pages, JHEP version, Appendix A expanded, one typo fixed