Correct Definition of the Gluon Fragmentation Function at High Energy Colliders

Since the definition of the gluon to hadrons fragmentation amplitude $<H,X\mathrm{\mid }g>$ involves gluon field $Q^{\mu a}(x)$ corresponding to single gluon incoming state $\mathrm{\mid }g>$, the present definition of the gluon fragmentation function at high energy colliders [which involves non-abelian field tensor $F^{\mu \nu a}(x)=\partial^\mu Q^{\nu a}(x) -\partial^\nu Q^{\mu a}(x)+gf^{abc}Q^{\mu b}(x)Q^{\nu c}(x)$insteadof$Q^{\mu a}(x)$ in the initial state] is not consistent with the single gluon incoming state $\mathrm{\mid }g>$. In this paper we derive the correct definition of the gluon fragmentation function at high energy colliders from first principles which is obtained from the single gluon incoming state $\mathrm{\mid }g>$ and is gauge invariant and is consistent with the factorization theorem in QCD.